@article{10067,
  abstract     = {The search for novel entangled phases of matter has lead to the recent discovery of a new class of “entanglement transitions,” exemplified by random tensor networks and monitored quantum circuits. Most known examples can be understood as some classical ordering transitions in an underlying statistical mechanics model, where entanglement maps onto the free-energy cost of inserting a domain wall. In this paper we study the possibility of entanglement transitions driven by physics beyond such statistical mechanics mappings. Motivated by recent applications of neural-network-inspired variational Ansätze, we investigate under what conditions on the variational parameters these Ansätze can capture an entanglement transition. We study the entanglement scaling of short-range restricted Boltzmann machine (RBM) quantum states with random phases. For uncorrelated random phases, we analytically demonstrate the absence of an entanglement transition and reveal subtle finite-size effects in finite-size numerical simulations. Introducing phases with correlations decaying as 1/r^α in real space, we observe three regions with a different scaling of entanglement entropy depending on the exponent α. We study the nature of the transition between these regions, finding numerical evidence for critical behavior. Our work establishes the presence of long-range correlated phases in RBM-based wave functions as a required ingredient for entanglement transitions.},
  author       = {Medina Ramos, Raimel A and Vasseur, Romain and Serbyn, Maksym},
  issn         = {2469-9969},
  journal      = {Physical Review B},
  number       = {10},
  publisher    = {American Physical Society},
  title        = {{Entanglement transitions from restricted Boltzmann machines}},
  doi          = {10.1103/physrevb.104.104205},
  volume       = {104},
  year         = {2021},
}

@article{10545,
  abstract     = {Classical models with complex energy landscapes represent a perspective avenue for the near-term application of quantum simulators. Until now, many theoretical works studied the performance of quantum algorithms for models with a unique ground state. However, when the classical problem is in a so-called clustering phase, the ground state manifold is highly degenerate. As an example, we consider a 3-XORSAT model defined on simple hypergraphs. The degeneracy of classical ground state manifold translates into the emergence of an extensive number of Z2 symmetries, which remain intact even in the presence of a quantum transverse magnetic field. We establish a general duality approach that restricts the quantum problem to a given sector of conserved Z2 charges and use it to study how the outcome of the quantum adiabatic algorithm depends on the hypergraph geometry. We show that the tree hypergraph which corresponds to a classically solvable instance of the 3-XORSAT problem features a constant gap, whereas the closed hypergraph encounters a second-order phase transition with a gap vanishing as a power-law in the problem size. The duality developed in this work provides a practical tool for studies of quantum models with classically degenerate energy manifold and reveals potential connections between glasses and gauge theories.},
  author       = {Medina Ramos, Raimel A and Serbyn, Maksym},
  issn         = {2469-9934},
  journal      = {Physical Review A},
  number       = {6},
  publisher    = {American Physical Society},
  title        = {{Duality approach to quantum annealing of the 3-variable exclusive-or satisfiability problem (3-XORSAT)}},
  doi          = {10.1103/physreva.104.062423},
  volume       = {104},
  year         = {2021},
}

@article{7553,
  abstract     = {Normative theories and statistical inference provide complementary approaches for the study of biological systems. A normative theory postulates that organisms have adapted to efficiently solve essential tasks, and proceeds to mathematically work out testable consequences of such optimality; parameters that maximize the hypothesized organismal function can be derived ab initio, without reference to experimental data. In contrast, statistical inference focuses on efficient utilization of data to learn model parameters, without reference to any a priori notion of biological function, utility, or fitness. Traditionally, these two approaches were developed independently and applied separately. Here we unify them in a coherent Bayesian framework that embeds a normative theory into a family of maximum-entropy “optimization priors.” This family defines a smooth interpolation between a data-rich inference regime (characteristic of “bottom-up” statistical models), and a data-limited ab inito prediction regime (characteristic of “top-down” normative theory). We demonstrate the applicability of our framework using data from the visual cortex, and argue that the flexibility it affords is essential to address a number of fundamental challenges relating to inference and prediction in complex, high-dimensional biological problems.},
  author       = {Mlynarski, Wiktor F and Hledik, Michal and Sokolowski, Thomas R and Tkačik, Gašper},
  journal      = {Neuron},
  number       = {7},
  pages        = {1227--1241.e5},
  publisher    = {Cell Press},
  title        = {{Statistical analysis and optimality of neural systems}},
  doi          = {10.1016/j.neuron.2021.01.020},
  volume       = {109},
  year         = {2021},
}

@article{9298,
  abstract     = {In 2008, we published the first set of guidelines for standardizing research in autophagy. Since then, this topic has received increasing attention, and many scientists have entered the field. Our knowledge base and relevant new technologies have also been expanding. Thus, it is important to formulate on a regular basis updated guidelines for monitoring autophagy in different organisms. Despite numerous reviews, there continues to be confusion regarding acceptable methods to evaluate autophagy, especially in multicellular eukaryotes. Here, we present a set of guidelines for investigators to select and interpret methods to examine autophagy and related processes, and for reviewers to provide realistic and reasonable critiques of reports that are focused on these processes. These guidelines are not meant to be a dogmatic set of rules, because the appropriateness of any assay largely depends on the question being asked and the system being used. Moreover, no individual assay is perfect for every situation, calling for the use of multiple techniques to properly monitor autophagy in each experimental setting. Finally, several core components of the autophagy machinery have been implicated in distinct autophagic processes (canonical and noncanonical autophagy), implying that genetic approaches to block autophagy should rely on targeting two or more autophagy-related genes that ideally participate in distinct steps of the pathway. Along similar lines, because multiple proteins involved in autophagy also regulate other cellular pathways including apoptosis, not all of them can be used as a specific marker for bona fide autophagic responses. Here, we critically discuss current methods of assessing autophagy and the information they can, or cannot, provide. Our ultimate goal is to encourage intellectual and technical innovation in the field. },
  author       = {Klionsky, Daniel J. and Abdel-Aziz, Amal Kamal and Abdelfatah, Sara and Abdellatif, Mahmoud and Abdoli, Asghar and Abel, Steffen and Abeliovich, Hagai and Abildgaard, Marie H. and Abudu, Yakubu Princely and Acevedo-Arozena, Abraham and Adamopoulos, Iannis E. and Adeli, Khosrow and Adolph, Timon E. and Adornetto, Annagrazia and Aflaki, Elma and Agam, Galila and Agarwal, Anupam and Aggarwal, Bharat B. and Agnello, Maria and Agostinis, Patrizia and Agrewala, Javed N. and Agrotis, Alexander and Aguilar, Patricia V. and Ahmad, S. Tariq and Ahmed, Zubair M. and Ahumada-Castro, Ulises and Aits, Sonja and Aizawa, Shu and Akkoc, Yunus and Akoumianaki, Tonia and Akpinar, Hafize Aysin and Al-Abd, Ahmed M. and Al-Akra, Lina and Al-Gharaibeh, Abeer and Alaoui-Jamali, Moulay A. and Alberti, Simon and Alcocer-Gómez, Elísabet and Alessandri, Cristiano and Ali, Muhammad and Alim Al-Bari, M. Abdul and Aliwaini, Saeb and Alizadeh, Javad and Almacellas, Eugènia and Almasan, Alexandru and Alonso, Alicia and Alonso, Guillermo D. and Altan-Bonnet, Nihal and Altieri, Dario C. and Álvarez, Élida M.C. and Alves, Sara and Alves Da Costa, Cristine and Alzaharna, Mazen M. and Amadio, Marialaura and Amantini, Consuelo and Amaral, Cristina and Ambrosio, Susanna and Amer, Amal O. and Ammanathan, Veena and An, Zhenyi and Andersen, Stig U. and Andrabi, Shaida A. and Andrade-Silva, Magaiver and Andres, Allen M. and Angelini, Sabrina and Ann, David and Anozie, Uche C. and Ansari, Mohammad Y. and Antas, Pedro and Antebi, Adam and Antón, Zuriñe and Anwar, Tahira and Apetoh, Lionel and Apostolova, Nadezda and Araki, Toshiyuki and Araki, Yasuhiro and Arasaki, Kohei and Araújo, Wagner L. and Araya, Jun and Arden, Catherine and Arévalo, Maria Angeles and Arguelles, Sandro and Arias, Esperanza and Arikkath, Jyothi and Arimoto, Hirokazu and Ariosa, Aileen R. and Armstrong-James, Darius and Arnauné-Pelloquin, Laetitia and Aroca, Angeles and Arroyo, Daniela S. and Arsov, Ivica and Artero, Rubén and Asaro, Dalia Maria Lucia and Aschner, Michael and Ashrafizadeh, Milad and Ashur-Fabian, Osnat and Atanasov, Atanas G. and Au, Alicia K. and Auberger, Patrick and Auner, Holger W. and Aurelian, Laure and Autelli, Riccardo and Avagliano, Laura and Ávalos, Yenniffer and Aveic, Sanja and Aveleira, Célia Alexandra and Avin-Wittenberg, Tamar and Aydin, Yucel and Ayton, Scott and Ayyadevara, Srinivas and Azzopardi, Maria and Baba, Misuzu and Backer, Jonathan M. and Backues, Steven K. and Bae, Dong Hun and Bae, Ok Nam and Bae, Soo Han and Baehrecke, Eric H. and Baek, Ahruem and Baek, Seung Hoon and Baek, Sung Hee and Bagetta, Giacinto and Bagniewska-Zadworna, Agnieszka and Bai, Hua and Bai, Jie and Bai, Xiyuan and Bai, Yidong and Bairagi, Nandadulal and Baksi, Shounak and Balbi, Teresa and Baldari, Cosima T. and Balduini, Walter and Ballabio, Andrea and Ballester, Maria and Balazadeh, Salma and Balzan, Rena and Bandopadhyay, Rina and Banerjee, Sreeparna and Banerjee, Sulagna and Bánréti, Ágnes and Bao, Yan and Baptista, Mauricio S. and Baracca, Alessandra and Barbati, Cristiana and Bargiela, Ariadna and Barilà, Daniela and Barlow, Peter G. and Barmada, Sami J. and Barreiro, Esther and Barreto, George E. and Bartek, Jiri and Bartel, Bonnie and Bartolome, Alberto and Barve, Gaurav R. and Basagoudanavar, Suresh H. and Bassham, Diane C. and Bast, Robert C. and Basu, Alakananda and Batoko, Henri and Batten, Isabella and Baulieu, Etienne E. and Baumgarner, Bradley L. and Bayry, Jagadeesh and Beale, Rupert and Beau, Isabelle and Beaumatin, Florian and Bechara, Luiz R.G. and Beck, George R. and Beers, Michael F. and Begun, Jakob and Behrends, Christian and Behrens, Georg M.N. and Bei, Roberto and Bejarano, Eloy and Bel, Shai and Behl, Christian and Belaid, Amine and Belgareh-Touzé, Naïma and Bellarosa, Cristina and Belleudi, Francesca and Belló Pérez, Melissa and Bello-Morales, Raquel and Beltran, Jackeline Soares De Oliveira and Beltran, Sebastián and Benbrook, Doris Mangiaracina and Bendorius, Mykolas and Benitez, Bruno A. and Benito-Cuesta, Irene and Bensalem, Julien and Berchtold, Martin W. and Berezowska, Sabina and Bergamaschi, Daniele and Bergami, Matteo and Bergmann, Andreas and Berliocchi, Laura and Berlioz-Torrent, Clarisse and Bernard, Amélie and Berthoux, Lionel and Besirli, Cagri G. and Besteiro, Sebastien and Betin, Virginie M. and Beyaert, Rudi and Bezbradica, Jelena S. and Bhaskar, Kiran and Bhatia-Kissova, Ingrid and Bhattacharya, Resham and Bhattacharya, Sujoy and Bhattacharyya, Shalmoli and Bhuiyan, Md Shenuarin and Bhutia, Sujit Kumar and Bi, Lanrong and Bi, Xiaolin and Biden, Trevor J. and Bijian, Krikor and Billes, Viktor A. and Binart, Nadine and Bincoletto, Claudia and Birgisdottir, Asa B. and Bjorkoy, Geir and Blanco, Gonzalo and Blas-Garcia, Ana and Blasiak, Janusz and Blomgran, Robert and Blomgren, Klas and Blum, Janice S. and Boada-Romero, Emilio and Boban, Mirta and Boesze-Battaglia, Kathleen and Boeuf, Philippe and Boland, Barry and Bomont, Pascale and Bonaldo, Paolo and Bonam, Srinivasa Reddy and Bonfili, Laura and Bonifacino, Juan S. and Boone, Brian A. and Bootman, Martin D. and Bordi, Matteo and Borner, Christoph and Bornhauser, Beat C. and Borthakur, Gautam and Bosch, Jürgen and Bose, Santanu and Botana, Luis M. and Botas, Juan and Boulanger, Chantal M. and Boulton, Michael E. and Bourdenx, Mathieu and Bourgeois, Benjamin and Bourke, Nollaig M. and Bousquet, Guilhem and Boya, Patricia and Bozhkov, Peter V. and Bozi, Luiz H.M. and Bozkurt, Tolga O. and Brackney, Doug E. and Brandts, Christian H. and Braun, Ralf J. and Braus, Gerhard H. and Bravo-Sagua, Roberto and Bravo-San Pedro, José M. and Brest, Patrick and Bringer, Marie Agnès and Briones-Herrera, Alfredo and Broaddus, V. Courtney and Brodersen, Peter and Brodsky, Jeffrey L. and Brody, Steven L. and Bronson, Paola G. and Bronstein, Jeff M. and Brown, Carolyn N. and Brown, Rhoderick E. and Brum, Patricia C. and Brumell, John H. and Brunetti-Pierri, Nicola and Bruno, Daniele and Bryson-Richardson, Robert J. and Bucci, Cecilia and Buchrieser, Carmen and Bueno, Marta and Buitrago-Molina, Laura Elisa and Buraschi, Simone and Buch, Shilpa and Buchan, J. Ross and Buckingham, Erin M. and Budak, Hikmet and Budini, Mauricio and Bultynck, Geert and Burada, Florin and Burgoyne, Joseph R. and Burón, M. Isabel and Bustos, Victor and Büttner, Sabrina and Butturini, Elena and Byrd, Aaron and Cabas, Isabel and Cabrera-Benitez, Sandra and Cadwell, Ken and Cai, Jingjing and Cai, Lu and Cai, Qian and Cairó, Montserrat and Calbet, Jose A. and Caldwell, Guy A. and Caldwell, Kim A. and Call, Jarrod A. and Calvani, Riccardo and Calvo, Ana C. and Calvo-Rubio Barrera, Miguel and Camara, Niels O.S. and Camonis, Jacques H. and Camougrand, Nadine and Campanella, Michelangelo and Campbell, Edward M. and Campbell-Valois, François Xavier and Campello, Silvia and Campesi, Ilaria and Campos, Juliane C. and Camuzard, Olivier and Cancino, Jorge and Candido De Almeida, Danilo and Canesi, Laura and Caniggia, Isabella and Canonico, Barbara and Cantí, Carles and Cao, Bin and Caraglia, Michele and Caramés, Beatriz and Carchman, Evie H. and Cardenal-Muñoz, Elena and Cardenas, Cesar and Cardenas, Luis and Cardoso, Sandra M. and Carew, Jennifer S. and Carle, Georges F. and Carleton, Gillian and Carloni, Silvia and Carmona-Gutierrez, Didac and Carneiro, Leticia A. and Carnevali, Oliana and Carosi, Julian M. and Carra, Serena and Carrier, Alice and Carrier, Lucie and Carroll, Bernadette and Carter, A. Brent and Carvalho, Andreia Neves and Casanova, Magali and Casas, Caty and Casas, Josefina and Cassioli, Chiara and Castillo, Eliseo F. and Castillo, Karen and Castillo-Lluva, Sonia and Castoldi, Francesca and Castori, Marco and Castro, Ariel F. and Castro-Caldas, Margarida and Castro-Hernandez, Javier and Castro-Obregon, Susana and Catz, Sergio D. and Cavadas, Claudia and Cavaliere, Federica and Cavallini, Gabriella and Cavinato, Maria and Cayuela, Maria L. and Cebollada Rica, Paula and Cecarini, Valentina and Cecconi, Francesco and Cechowska-Pasko, Marzanna and Cenci, Simone and Ceperuelo-Mallafré, Victòria and Cerqueira, João J. and Cerutti, Janete M. and Cervia, Davide and Cetintas, Vildan Bozok and Cetrullo, Silvia and Chae, Han Jung and Chagin, Andrei S. and Chai, Chee Yin and Chakrabarti, Gopal and Chakrabarti, Oishee and Chakraborty, Tapas and Chakraborty, Trinad and Chami, Mounia and Chamilos, Georgios and Chan, David W. and Chan, Edmond Y.W. and Chan, Edward D. and Chan, H. Y.Edwin and Chan, Helen H. and Chan, Hung and Chan, Matthew T.V. and Chan, Yau Sang and Chandra, Partha K. and Chang, Chih Peng and Chang, Chunmei and Chang, Hao Chun and Chang, Kai and Chao, Jie and Chapman, Tracey and Charlet-Berguerand, Nicolas and Chatterjee, Samrat and Chaube, Shail K. and Chaudhary, Anu and Chauhan, Santosh and Chaum, Edward and Checler, Frédéric and Cheetham, Michael E. and Chen, Chang Shi and Chen, Guang Chao and Chen, Jian Fu and Chen, Liam L. and Chen, Leilei and Chen, Lin and Chen, Mingliang and Chen, Mu Kuan and Chen, Ning and Chen, Quan and Chen, Ruey Hwa and Chen, Shi and Chen, Wei and Chen, Weiqiang and Chen, Xin Ming and Chen, Xiong Wen and Chen, Xu and Chen, Yan and Chen, Ye Guang and Chen, Yingyu and Chen, Yongqiang and Chen, Yu Jen and Chen, Yue Qin and Chen, Zhefan Stephen and Chen, Zhi and Chen, Zhi Hua and Chen, Zhijian J. and Chen, Zhixiang and Cheng, Hanhua and Cheng, Jun and Cheng, Shi Yuan and Cheng, Wei and Cheng, Xiaodong and Cheng, Xiu Tang and Cheng, Yiyun and Cheng, Zhiyong and Chen, Zhong and Cheong, Heesun and Cheong, Jit Kong and Chernyak, Boris V. and Cherry, Sara and Cheung, Chi Fai Randy and Cheung, Chun Hei Antonio and Cheung, King Ho and Chevet, Eric and Chi, Richard J. and Chiang, Alan Kwok Shing and Chiaradonna, Ferdinando and Chiarelli, Roberto and Chiariello, Mario and Chica, Nathalia and Chiocca, Susanna and Chiong, Mario and Chiou, Shih Hwa and Chiramel, Abhilash I. and Chiurchiù, Valerio and Cho, Dong Hyung and Choe, Seong Kyu and Choi, Augustine M.K. and Choi, Mary E. and Choudhury, Kamalika Roy and Chow, Norman S. and Chu, Charleen T. and Chua, Jason P. and Chua, John Jia En and Chung, Hyewon and Chung, Kin Pan and Chung, Seockhoon and Chung, So Hyang and Chung, Yuen Li and Cianfanelli, Valentina and Ciechomska, Iwona A. and Cifuentes, Mariana and Cinque, Laura and Cirak, Sebahattin and Cirone, Mara and Clague, Michael J. and Clarke, Robert and Clementi, Emilio and Coccia, Eliana M. and Codogno, Patrice and Cohen, Ehud and Cohen, Mickael M. and Colasanti, Tania and Colasuonno, Fiorella and Colbert, Robert A. and Colell, Anna and Čolić, Miodrag and Coll, Nuria S. and Collins, Mark O. and Colombo, María I. and Colón-Ramos, Daniel A. and Combaret, Lydie and Comincini, Sergio and Cominetti, Márcia R. and Consiglio, Antonella and Conte, Andrea and Conti, Fabrizio and Contu, Viorica Raluca and Cookson, Mark R. and Coombs, Kevin M. and Coppens, Isabelle and Corasaniti, Maria Tiziana and Corkery, Dale P. and Cordes, Nils and Cortese, Katia and Costa, Maria Do Carmo and Costantino, Sarah and Costelli, Paola and Coto-Montes, Ana and Crack, Peter J. and Crespo, Jose L. and Criollo, Alfredo and Crippa, Valeria and Cristofani, Riccardo and Csizmadia, Tamas and Cuadrado, Antonio and Cui, Bing and Cui, Jun and Cui, Yixian and Cui, Yong and Culetto, Emmanuel and Cumino, Andrea C. and Cybulsky, Andrey V. and Czaja, Mark J. and Czuczwar, Stanislaw J. and D’Adamo, Stefania and D’Amelio, Marcello and D’Arcangelo, Daniela and D’Lugos, Andrew C. and D’Orazi, Gabriella and Da Silva, James A. and Dafsari, Hormos Salimi and Dagda, Ruben K. and Dagdas, Yasin and Daglia, Maria and Dai, Xiaoxia and Dai, Yun and Dai, Yuyuan and Dal Col, Jessica and Dalhaimer, Paul and Dalla Valle, Luisa and Dallenga, Tobias and Dalmasso, Guillaume and Damme, Markus and Dando, Ilaria and Dantuma, Nico P. and Darling, April L. and Das, Hiranmoy and Dasarathy, Srinivasan and Dasari, Santosh K. and Dash, Srikanta and Daumke, Oliver and Dauphinee, Adrian N. and Davies, Jeffrey S. and Dávila, Valeria A. and Davis, Roger J. and Davis, Tanja and Dayalan Naidu, Sharadha and De Amicis, Francesca and De Bosscher, Karolien and De Felice, Francesca and De Franceschi, Lucia and De Leonibus, Chiara and De Mattos Barbosa, Mayara G. and De Meyer, Guido R.Y. and De Milito, Angelo and De Nunzio, Cosimo and De Palma, Clara and De Santi, Mauro and De Virgilio, Claudio and De Zio, Daniela and Debnath, Jayanta and Debosch, Brian J. and Decuypere, Jean Paul and Deehan, Mark A. and Deflorian, Gianluca and Degregori, James and Dehay, Benjamin and Del Rio, Gabriel and Delaney, Joe R. and Delbridge, Lea M.D. and Delorme-Axford, Elizabeth and Delpino, M. Victoria and Demarchi, Francesca and Dembitz, Vilma and Demers, Nicholas D. and Deng, Hongbin and Deng, Zhiqiang and Dengjel, Joern and Dent, Paul and Denton, Donna and Depamphilis, Melvin L. and Der, Channing J. and Deretic, Vojo and Descoteaux, Albert and Devis, Laura and Devkota, Sushil and Devuyst, Olivier and Dewson, Grant and Dharmasivam, Mahendiran and Dhiman, Rohan and Di Bernardo, Diego and Di Cristina, Manlio and Di Domenico, Fabio and Di Fazio, Pietro and Di Fonzo, Alessio and Di Guardo, Giovanni and Di Guglielmo, Gianni M. and Di Leo, Luca and Di Malta, Chiara and Di Nardo, Alessia and Di Rienzo, Martina and Di Sano, Federica and Diallinas, George and Diao, Jiajie and Diaz-Araya, Guillermo and Díaz-Laviada, Inés and Dickinson, Jared M. and Diederich, Marc and Dieudé, Mélanie and Dikic, Ivan and Ding, Shiping and Ding, Wen Xing and Dini, Luciana and Dinić, Jelena and Dinic, Miroslav and Dinkova-Kostova, Albena T. and Dionne, Marc S. and Distler, Jörg H.W. and Diwan, Abhinav and Dixon, Ian M.C. and Djavaheri-Mergny, Mojgan and Dobrinski, Ina and Dobrovinskaya, Oxana and Dobrowolski, Radek and Dobson, Renwick C.J. and Đokić, Jelena and Dokmeci Emre, Serap and Donadelli, Massimo and Dong, Bo and Dong, Xiaonan and Dong, Zhiwu and Dorn, Gerald W. and Dotsch, Volker and Dou, Huan and Dou, Juan and Dowaidar, Moataz and Dridi, Sami and Drucker, Liat and Du, Ailian and Du, Caigan and Du, Guangwei and Du, Hai Ning and Du, Li Lin and Du Toit, André and Duan, Shao Bin and Duan, Xiaoqiong and Duarte, Sónia P. and Dubrovska, Anna and Dunlop, Elaine A. and Dupont, Nicolas and Durán, Raúl V. and Dwarakanath, Bilikere S. and Dyshlovoy, Sergey A. and Ebrahimi-Fakhari, Darius and Eckhart, Leopold and Edelstein, Charles L. and Efferth, Thomas and Eftekharpour, Eftekhar and Eichinger, Ludwig and Eid, Nabil and Eisenberg, Tobias and Eissa, N. Tony and Eissa, Sanaa and Ejarque, Miriam and El Andaloussi, Abdeljabar and El-Hage, Nazira and El-Naggar, Shahenda and Eleuteri, Anna Maria and El-Shafey, Eman S. and Elgendy, Mohamed and Eliopoulos, Aristides G. and Elizalde, María M. and Elks, Philip M. and Elsasser, Hans Peter and Elsherbiny, Eslam S. and Emerling, Brooke M. and Emre, N. C.Tolga and Eng, Christina H. and Engedal, Nikolai and Engelbrecht, Anna Mart and Engelsen, Agnete S.T. and Enserink, Jorrit M. and Escalante, Ricardo and Esclatine, Audrey and Escobar-Henriques, Mafalda and Eskelinen, Eeva Liisa and Espert, Lucile and Eusebio, Makandjou Ola and Fabrias, Gemma and Fabrizi, Cinzia and Facchiano, Antonio and Facchiano, Francesco and Fadeel, Bengt and Fader, Claudio and Faesen, Alex C. and Fairlie, W. Douglas and Falcó, Alberto and Falkenburger, Bjorn H. and Fan, Daping and Fan, Jie and Fan, Yanbo and Fang, Evandro F. and Fang, Yanshan and Fang, Yognqi and Fanto, Manolis and Farfel-Becker, Tamar and Faure, Mathias and Fazeli, Gholamreza and Fedele, Anthony O. and Feldman, Arthur M. and Feng, Du and Feng, Jiachun and Feng, Lifeng and Feng, Yibin and Feng, Yuchen and Feng, Wei and Fenz Araujo, Thais and Ferguson, Thomas A. and Fernández, Álvaro F. and Fernandez-Checa, Jose C. and Fernández-Veledo, Sonia and Fernie, Alisdair R. and Ferrante, Anthony W. and Ferraresi, Alessandra and Ferrari, Merari F. and Ferreira, Julio C.B. and Ferro-Novick, Susan and Figueras, Antonio and Filadi, Riccardo and Filigheddu, Nicoletta and Filippi-Chiela, Eduardo and Filomeni, Giuseppe and Fimia, Gian Maria and Fineschi, Vittorio and Finetti, Francesca and Finkbeiner, Steven and Fisher, Edward A. and Fisher, Paul B. and Flamigni, Flavio and Fliesler, Steven J. and Flo, Trude H. and Florance, Ida and Florey, Oliver and Florio, Tullio and Fodor, Erika and Follo, Carlo and Fon, Edward A. and Forlino, Antonella and Fornai, Francesco and Fortini, Paola and Fracassi, Anna and Fraldi, Alessandro and Franco, Brunella and Franco, Rodrigo and Franconi, Flavia and Frankel, Lisa B. and Friedman, Scott L. and Fröhlich, Leopold F. and Frühbeck, Gema and Fuentes, Jose M. and Fujiki, Yukio and Fujita, Naonobu and Fujiwara, Yuuki and Fukuda, Mitsunori and Fulda, Simone and Furic, Luc and Furuya, Norihiko and Fusco, Carmela and Gack, Michaela U. and Gaffke, Lidia and Galadari, Sehamuddin and Galasso, Alessia and Galindo, Maria F. and Gallolu Kankanamalage, Sachith and Galluzzi, Lorenzo and Galy, Vincent and Gammoh, Noor and Gan, Boyi and Ganley, Ian G. and Gao, Feng and Gao, Hui and Gao, Minghui and Gao, Ping and Gao, Shou Jiang and Gao, Wentao and Gao, Xiaobo and Garcera, Ana and Garcia, Maria Noé and Garcia, Verónica E. and García-Del Portillo, Francisco and Garcia-Escudero, Vega and Garcia-Garcia, Aracely and Garcia-Macia, Marina and García-Moreno, Diana and Garcia-Ruiz, Carmen and García-Sanz, Patricia and Garg, Abhishek D. and Gargini, Ricardo and Garofalo, Tina and Garry, Robert F. and Gassen, Nils C. and Gatica, Damian and Ge, Liang and Ge, Wanzhong and Geiss-Friedlander, Ruth and Gelfi, Cecilia and Genschik, Pascal and Gentle, Ian E. and Gerbino, Valeria and Gerhardt, Christoph and Germain, Kyla and Germain, Marc and Gewirtz, David A. and Ghasemipour Afshar, Elham and Ghavami, Saeid and Ghigo, Alessandra and Ghosh, Manosij and Giamas, Georgios and Giampietri, Claudia and Giatromanolaki, Alexandra and Gibson, Gary E. and Gibson, Spencer B. and Ginet, Vanessa and Giniger, Edward and Giorgi, Carlotta and Girao, Henrique and Girardin, Stephen E. and Giridharan, Mridhula and Giuliano, Sandy and Giulivi, Cecilia and Giuriato, Sylvie and Giustiniani, Julien and Gluschko, Alexander and Goder, Veit and Goginashvili, Alexander and Golab, Jakub and Goldstone, David C. and Golebiewska, Anna and Gomes, Luciana R. and Gomez, Rodrigo and Gómez-Sánchez, Rubén and Gomez-Puerto, Maria Catalina and Gomez-Sintes, Raquel and Gong, Qingqiu and Goni, Felix M. and González-Gallego, Javier and Gonzalez-Hernandez, Tomas and Gonzalez-Polo, Rosa A. and Gonzalez-Reyes, Jose A. and González-Rodríguez, Patricia and Goping, Ing Swie and Gorbatyuk, Marina S. and Gorbunov, Nikolai V. and Görgülü, Kıvanç and Gorojod, Roxana M. and Gorski, Sharon M. and Goruppi, Sandro and Gotor, Cecilia and Gottlieb, Roberta A. and Gozes, Illana and Gozuacik, Devrim and Graef, Martin and Gräler, Markus H. and Granatiero, Veronica and Grasso, Daniel and Gray, Joshua P. and Green, Douglas R. and Greenhough, Alexander and Gregory, Stephen L. and Griffin, Edward F. and Grinstaff, Mark W. and Gros, Frederic and Grose, Charles and Gross, Angelina S. and Gruber, Florian and Grumati, Paolo and Grune, Tilman and Gu, Xueyan and Guan, Jun Lin and Guardia, Carlos M. and Guda, Kishore and Guerra, Flora and Guerri, Consuelo and Guha, Prasun and Guillén, Carlos and Gujar, Shashi and Gukovskaya, Anna and Gukovsky, Ilya and Gunst, Jan and Günther, Andreas and Guntur, Anyonya R. and Guo, Chuanyong and Guo, Chun and Guo, Hongqing and Guo, Lian Wang and Guo, Ming and Gupta, Pawan and Gupta, Shashi Kumar and Gupta, Swapnil and Gupta, Veer Bala and Gupta, Vivek and Gustafsson, Asa B. and Gutterman, David D. and H.B, Ranjitha and Haapasalo, Annakaisa and Haber, James E. and Hać, Aleksandra and Hadano, Shinji and Hafrén, Anders J. and Haidar, Mansour and Hall, Belinda S. and Halldén, Gunnel and Hamacher-Brady, Anne and Hamann, Andrea and Hamasaki, Maho and Han, Weidong and Hansen, Malene and Hanson, Phyllis I. . and Hao, Zijian and Harada, Masaru and Harhaji-Trajkovic, Ljubica and Hariharan, Nirmala and Haroon, Nigil and Harris, James and Hasegawa, Takafumi and Hasima Nagoor, Noor and Haspel, Jeffrey A. and Haucke, Volker and Hawkins, Wayne D. and Hay, Bruce A. and Haynes, Cole M. and Hayrabedyan, Soren B. and Hays, Thomas S. and He, Congcong and He, Qin and He, Rong Rong and He, You Wen and He, Yu Ying and Heakal, Yasser and Heberle, Alexander M. and Hejtmancik, J. 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and Kanthasamy, Anumantha G. and Kanthasamy, Arthi and Kantorow, Marc and Kapuy, Orsolya and Karamouzis, Michalis V. and Karim, Md Razaul and Karmakar, Parimal and Katare, Rajesh G. and Kato, Masaru and Kaufmann, Stefan H.E. and Kauppinen, Anu and Kaushal, Gur P. and Kaushik, Susmita and Kawasaki, Kiyoshi and Kazan, Kemal and Ke, Po Yuan and Keating, Damien J. and Keber, Ursula and Kehrl, John H. and Keller, Kate E. and Keller, Christian W. and Kemper, Jongsook Kim and Kenific, Candia M. and Kepp, Oliver and Kermorgant, Stephanie and Kern, Andreas and Ketteler, Robin and Keulers, Tom G. and Khalfin, Boris and Khalil, Hany and Khambu, Bilon and Khan, Shahid Y. and Khandelwal, Vinoth Kumar Megraj and Khandia, Rekha and Kho, Widuri and Khobrekar, Noopur V. and Khuansuwan, Sataree and Khundadze, Mukhran and Killackey, Samuel A. and Kim, Dasol and Kim, Deok Ryong and Kim, Do Hyung and Kim, Dong Eun and Kim, Eun Young and Kim, Eun Kyoung and Kim, Hak Rim and Kim, Hee Sik and Hyung-Ryong Kim, Unknown and Kim, Jeong Hun and Kim, Jin Kyung and Kim, Jin Hoi and Kim, Joungmok and Kim, Ju Hwan and Kim, Keun Il and Kim, Peter K. and Kim, Seong Jun and Kimball, Scot R. and Kimchi, Adi and Kimmelman, Alec C. and Kimura, Tomonori and King, Matthew A. and Kinghorn, Kerri J. and Kinsey, Conan G. and Kirkin, Vladimir and Kirshenbaum, Lorrie A. and Kiselev, Sergey L. and Kishi, Shuji and Kitamoto, Katsuhiko and Kitaoka, Yasushi and Kitazato, Kaio and Kitsis, Richard N. and Kittler, Josef T. and Kjaerulff, Ole and Klein, Peter S. and Klopstock, Thomas and Klucken, Jochen and Knævelsrud, Helene and Knorr, Roland L. and Ko, Ben C.B. and Ko, Fred and Ko, Jiunn Liang and Kobayashi, Hotaka and Kobayashi, Satoru and Koch, Ina and Koch, Jan C. and Koenig, Ulrich and Kögel, Donat and Koh, Young Ho and Koike, Masato and Kohlwein, Sepp D. and Kocaturk, Nur M. and Komatsu, Masaaki and König, Jeannette and Kono, Toru and Kopp, Benjamin T. and Korcsmaros, Tamas and Korkmaz, Gözde and Korolchuk, 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Guanghong and Liao, Lujian and Liao, Mingzhi and Liao, Yung Feng and Librizzi, Mariangela and Lie, Pearl P.Y. and Lilly, Mary A. and Lim, Hyunjung J. and Lima, Thania R.R. and Limana, Federica and Lin, Chao and Lin, Chih Wen and Lin, Dar Shong and Lin, Fu Cheng and Lin, Jiandie D. and Lin, Kurt M. and Lin, Kwang Huei and Lin, Liang Tzung and Lin, Pei Hui and Lin, Qiong and Lin, Shaofeng and Lin, Su Ju and Lin, Wenyu and Lin, Xueying and Lin, Yao Xin and Lin, Yee Shin and Linden, Rafael and Lindner, Paula and Ling, Shuo Chien and Lingor, Paul and Linnemann, Amelia K. and Liou, Yih Cherng and Lipinski, Marta M. and Lipovšek, Saška and Lira, Vitor A. and Lisiak, Natalia and Liton, Paloma B. and Liu, Chao and Liu, Ching Hsuan and Liu, Chun Feng and Liu, Cui Hua and Liu, Fang and Liu, Hao and Liu, Hsiao Sheng and Liu, Hua Feng and Liu, Huifang and Liu, Jia and Liu, Jing and Liu, Julia and Liu, Leyuan and Liu, Longhua and Liu, Meilian and Liu, Qin and Liu, Wei and Liu, Wende and Liu, Xiao 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and Manjili, Masoud H. and Manjithaya, Ravi and Manque, Patricio and Manshian, Bella B. and Manzano, Raquel and Manzoni, Claudia and Mao, Kai and Marchese, Cinzia and Marchetti, Sandrine and Marconi, Anna Maria and Marcucci, Fabrizio and Mardente, Stefania and Mareninova, Olga A. and Margeta, Marta and Mari, Muriel and Marinelli, Sara and Marinelli, Oliviero and Mariño, Guillermo and Mariotto, Sofia and Marshall, Richard S. and Marten, Mark R. and Martens, Sascha and Martin, Alexandre P.J. and Martin, Katie R. and Martin, Sara and Martin, Shaun and Martín-Segura, Adrián and Martín-Acebes, Miguel A. and Martin-Burriel, Inmaculada and Martin-Rincon, Marcos and Martin-Sanz, Paloma and Martina, José A. and Martinet, Wim and Martinez, Aitor and Martinez, Ana and Martinez, Jennifer and Martinez Velazquez, Moises and Martinez-Lopez, Nuria and Martinez-Vicente, Marta and Martins, Daniel O. and Martins, Joilson O. and Martins, Waleska K. and Martins-Marques, Tania and Marzetti, Emanuele and 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Patrick and Murthy, Aditya and Myöhänen, Timo T. and Mysorekar, Indira U. and Mytych, Jennifer and Nabavi, Seyed Mohammad and Nabissi, Massimo and Nagy, Péter and Nah, Jihoon and Nahimana, Aimable and Nakagawa, Ichiro and Nakamura, Ken and Nakatogawa, Hitoshi and Nandi, Shyam S. and Nanjundan, Meera and Nanni, Monica and Napolitano, Gennaro and Nardacci, Roberta and Narita, Masashi and Nassif, Melissa and Nathan, Ilana and Natsumeda, Manabu and Naude, Ryno J. and Naumann, Christin and Naveiras, Olaia and Navid, Fatemeh and Nawrocki, Steffan T. and Nazarko, Taras Y. and Nazio, Francesca and Negoita, Florentina and Neill, Thomas and Neisch, Amanda L. and Neri, Luca M. and Netea, Mihai G. and Neubert, Patrick and Neufeld, Thomas P. and Neumann, Dietbert and Neutzner, Albert and Newton, Phillip T. and Ney, Paul A. and Nezis, Ioannis P. and Ng, Charlene C.W. and Ng, Tzi Bun and Nguyen, Hang T.T. and Nguyen, Long T. and Ni, Hong Min and Ní Cheallaigh, Clíona and Ni, Zhenhong and Nicolao, M. Celeste and Nicoli, Francesco and Nieto-Diaz, Manuel and Nilsson, Per and Ning, Shunbin and Niranjan, Rituraj and Nishimune, Hiroshi and Niso-Santano, Mireia and Nixon, Ralph A. and Nobili, Annalisa and Nobrega, Clevio and Noda, Takeshi and Nogueira-Recalde, Uxía and Nolan, Trevor M. and Nombela, Ivan and Novak, Ivana and Novoa, Beatriz and Nozawa, Takashi and Nukina, Nobuyuki and Nussbaum-Krammer, Carmen and Nylandsted, Jesper and O’Donovan, Tracey R. and O’Leary, Seónadh M. and O’Rourke, Eyleen J. and O’Sullivan, Mary P. and O’Sullivan, Timothy E. and Oddo, Salvatore and Oehme, Ina and Ogawa, Michinaga and Ogier-Denis, Eric and Ogmundsdottir, Margret H. and Ogretmen, Besim and Oh, Goo Taeg and Oh, Seon Hee and Oh, Young J. and Ohama, Takashi and Ohashi, Yohei and Ohmuraya, Masaki and Oikonomou, Vasileios and Ojha, Rani and Okamoto, Koji and Okazawa, Hitoshi and Oku, Masahide and Oliván, Sara and Oliveira, Jorge M.A. and Ollmann, Michael and Olzmann, James A. and Omari, Shakib and Omary, M. 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Wei Lynn and Wu, An Guo and Wu, Chengbiao and Wu, Jian and Wu, Junfang and Wu, Kenneth K. and Wu, Min and Wu, Shan Ying and Wu, Shengzhou and Wu, Shu Yan and Wu, Shufang and Wu, William K.K. and Wu, Xiaohong and Wu, Xiaoqing and Wu, Yao Wen and Wu, Yihua and Xavier, Ramnik J. and Xia, Hongguang and Xia, Lixin and Xia, Zhengyuan and Xiang, Ge and Xiang, Jin and Xiang, Mingliang and Xiang, Wei and Xiao, Bin and Xiao, Guozhi and Xiao, Hengyi and Xiao, Hong Tao and Xiao, Jian and Xiao, Lan and Xiao, Shi and Xiao, Yin and Xie, Baoming and Xie, Chuan Ming and Xie, Min and Xie, Yuxiang and Xie, Zhiping and Xie, Zhonglin and Xilouri, Maria and Xu, Congfeng and Xu, En and Xu, Haoxing and Xu, Jing and Xu, Jin Rong and Xu, Liang and Xu, Wen Wen and Xu, Xiulong and Xue, Yu and Yakhine-Diop, Sokhna M.S. and Yamaguchi, Masamitsu and Yamaguchi, Osamu and Yamamoto, Ai and Yamashina, Shunhei and Yan, Shengmin and Yan, Shian Jang and Yan, Zhen and Yanagi, Yasuo and Yang, Chuanbin and Yang, Dun Sheng and Yang, Huan and Yang, Huang Tian and Yang, Hui and Yang, Jin Ming and Yang, Jing and Yang, Jingyu and Yang, Ling and Yang, Liu and Yang, Ming and Yang, Pei Ming and Yang, Qian and Yang, Seungwon and Yang, Shu and Yang, Shun Fa and Yang, Wannian and Yang, Wei Yuan and Yang, Xiaoyong and Yang, Xuesong and Yang, Yi and Yang, Ying and Yao, Honghong and Yao, Shenggen and Yao, Xiaoqiang and Yao, Yong Gang and Yao, Yong Ming and Yasui, Takahiro and Yazdankhah, Meysam and Yen, Paul M. and Yi, Cong and Yin, Xiao Ming and Yin, Yanhai and Yin, Zhangyuan and Yin, Ziyi and Ying, Meidan and Ying, Zheng and Yip, Calvin K. and Yiu, Stephanie Pei Tung and Yoo, Young H. and Yoshida, Kiyotsugu and Yoshii, Saori R. and Yoshimori, Tamotsu and Yousefi, Bahman and Yu, Boxuan and Yu, Haiyang and Yu, Jun and Yu, Jun and Yu, Li and Yu, Ming Lung and Yu, Seong Woon and Yu, Victor C. and Yu, W. Haung and Yu, Zhengping and Yu, Zhou and Yuan, Junying and Yuan, Ling Qing and Yuan, Shilin and Yuan, Shyng Shiou F. and Yuan, Yanggang and Yuan, Zengqiang and Yue, Jianbo and Yue, Zhenyu and Yun, Jeanho and Yung, Raymond L. and Zacks, David N. and Zaffagnini, Gabriele and Zambelli, Vanessa O. and Zanella, Isabella and Zang, Qun S. and Zanivan, Sara and Zappavigna, Silvia and Zaragoza, Pilar and Zarbalis, Konstantinos S. and Zarebkohan, Amir and Zarrouk, Amira and Zeitlin, Scott O. and Zeng, Jialiu and Zeng, Ju Deng and Žerovnik, Eva and Zhan, Lixuan and Zhang, Bin and Zhang, Donna D. and Zhang, Hanlin and Zhang, Hong and Zhang, Hong and Zhang, Honghe and Zhang, Huafeng and Zhang, Huaye and Zhang, Hui and Zhang, Hui Ling and Zhang, Jianbin and Zhang, Jianhua and Zhang, Jing Pu and Zhang, Kalin Y.B. and Zhang, Leshuai W. and Zhang, Lin and Zhang, Lisheng and Zhang, Lu and Zhang, Luoying and Zhang, Menghuan and Zhang, Peng and Zhang, Sheng and Zhang, Wei and Zhang, Xiangnan and Zhang, Xiao Wei and Zhang, Xiaolei and Zhang, Xiaoyan and Zhang, Xin and Zhang, Xinxin and Zhang, Xu Dong and Zhang, Yang and Zhang, Yanjin and Zhang, Yi and Zhang, Ying Dong and Zhang, Yingmei and Zhang, Yuan Yuan and Zhang, Yuchen and Zhang, Zhe and Zhang, Zhengguang and Zhang, Zhibing and Zhang, Zhihai and Zhang, Zhiyong and Zhang, Zili and Zhao, Haobin and Zhao, Lei and Zhao, Shuang and Zhao, Tongbiao and Zhao, Xiao Fan and Zhao, Ying and Zhao, Yongchao and Zhao, Yongliang and Zhao, Yuting and Zheng, Guoping and Zheng, Kai and Zheng, Ling and Zheng, Shizhong and Zheng, Xi Long and Zheng, Yi and Zheng, Zu Guo and Zhivotovsky, Boris and Zhong, Qing and Zhou, Ao and Zhou, Ben and Zhou, Cefan and Zhou, Gang and Zhou, Hao and Zhou, Hong and Zhou, Hongbo and Zhou, Jie and Zhou, Jing and Zhou, Jing and Zhou, Jiyong and Zhou, Kailiang and Zhou, Rongjia and Zhou, Xu Jie and Zhou, Yanshuang and Zhou, Yinghong and Zhou, Yubin and Zhou, Zheng Yu and Zhou, Zhou and Zhu, Binglin and Zhu, Changlian and Zhu, Guo Qing and Zhu, Haining and Zhu, Hongxin and Zhu, Hua and Zhu, Wei Guo and Zhu, Yanping and Zhu, Yushan and Zhuang, Haixia and Zhuang, Xiaohong and Zientara-Rytter, Katarzyna and Zimmermann, Christine M. and Ziviani, Elena and Zoladek, Teresa and Zong, Wei Xing and Zorov, Dmitry B. and Zorzano, Antonio and Zou, Weiping and Zou, Zhen and Zou, Zhengzhi and Zuryn, Steven and Zwerschke, Werner and Brand-Saberi, Beate and Dong, X. Charlie and Kenchappa, Chandra Shekar and Li, Zuguo and Lin, Yong and Oshima, Shigeru and Rong, Yueguang and Sluimer, Judith C. and Stallings, Christina L. and Tong, Chun Kit},
  issn         = {1554-8635},
  journal      = {Autophagy},
  number       = {1},
  pages        = {1--382},
  publisher    = {Taylor & Francis},
  title        = {{Guidelines for the use and interpretation of assays for monitoring autophagy (4th edition)}},
  doi          = {10.1080/15548627.2020.1797280},
  volume       = {17},
  year         = {2021},
}

@inproceedings{12909,
  author       = {Schlögl, Alois and Elefante, Stefano and Hornoiu, Andrei and Stadlbauer, Stephan},
  booktitle    = {ASHPC21 – Austrian-Slovenian HPC Meeting 2021},
  isbn         = {978-961-6980-77-7},
  location     = {Virtual},
  pages        = {5},
  publisher    = {University of Ljubljana},
  title        = {{Managing software on a heterogenous HPC cluster}},
  doi          = {10.3359/2021hpc},
  year         = {2021},
}

@inproceedings{10004,
  abstract     = {Markov chains are the de facto finite-state model for stochastic dynamical systems, and Markov decision processes (MDPs) extend Markov chains by incorporating non-deterministic behaviors. Given an MDP and rewards on states, a classical optimization criterion is the maximal expected total reward where the MDP stops after T steps, which can be computed by a simple dynamic programming algorithm. We consider a natural generalization of the problem where the stopping times can be chosen according to a probability distribution, such that the expected stopping time is T, to optimize the expected total reward. Quite surprisingly we establish inter-reducibility of the expected stopping-time problem for Markov chains with the Positivity problem (which is related to the well-known Skolem problem), for which establishing either decidability or undecidability would be a major breakthrough. Given the hardness of the exact problem, we consider the approximate version of the problem: we show that it can be solved in exponential time for Markov chains and in exponential space for MDPs.},
  author       = {Chatterjee, Krishnendu and Doyen, Laurent},
  booktitle    = {Proceedings of the 36th Annual ACM/IEEE Symposium on Logic in Computer Science},
  isbn         = {978-1-6654-4896-3},
  issn         = {1043-6871},
  keywords     = {Computer science, Heuristic algorithms, Memory management, Automata, Markov processes, Probability distribution, Complexity theory},
  location     = {Rome, Italy},
  pages        = {1--13},
  publisher    = {IEEE},
  title        = {{Stochastic processes with expected stopping time}},
  doi          = {10.1109/LICS52264.2021.9470595},
  year         = {2021},
}

@inproceedings{10408,
  abstract     = {Key trees are often the best solution in terms of transmission cost and storage requirements for managing keys in a setting where a group needs to share a secret key, while being able to efficiently rotate the key material of users (in order to recover from a potential compromise, or to add or remove users). Applications include multicast encryption protocols like LKH (Logical Key Hierarchies) or group messaging like the current IETF proposal TreeKEM. A key tree is a (typically balanced) binary tree, where each node is identified with a key: leaf nodes hold users’ secret keys while the root is the shared group key. For a group of size N, each user just holds   log(N)  keys (the keys on the path from its leaf to the root) and its entire key material can be rotated by broadcasting   2log(N)  ciphertexts (encrypting each fresh key on the path under the keys of its parents). In this work we consider the natural setting where we have many groups with partially overlapping sets of users, and ask if we can find solutions where the cost of rotating a key is better than in the trivial one where we have a separate key tree for each group. We show that in an asymptotic setting (where the number m of groups is fixed while the number N of users grows) there exist more general key graphs whose cost converges to the cost of a single group, thus saving a factor linear in the number of groups over the trivial solution. As our asymptotic “solution” converges very slowly and performs poorly on concrete examples, we propose an algorithm that uses a natural heuristic to compute a key graph for any given group structure. Our algorithm combines two greedy algorithms, and is thus very efficient: it first converts the group structure into a “lattice graph”, which is then turned into a key graph by repeatedly applying the algorithm for constructing a Huffman code. To better understand how far our proposal is from an optimal solution, we prove lower bounds on the update cost of continuous group-key agreement and multicast encryption in a symbolic model admitting (asymmetric) encryption, pseudorandom generators, and secret sharing as building blocks.},
  author       = {Alwen, Joel F and Auerbach, Benedikt and Baig, Mirza Ahad and Cueto Noval, Miguel and Klein, Karen and Pascual Perez, Guillermo and Pietrzak, Krzysztof Z and Walter, Michael},
  booktitle    = {19th International Conference},
  isbn         = {9-783-0309-0455-5},
  issn         = {1611-3349},
  location     = {Raleigh, NC, United States},
  pages        = {222--253},
  publisher    = {Springer Nature},
  title        = {{Grafting key trees: Efficient key management for overlapping groups}},
  doi          = {10.1007/978-3-030-90456-2_8},
  volume       = {13044},
  year         = {2021},
}

@inproceedings{10049,
  abstract     = {While messaging systems with strong security guarantees are widely used in practice, designing a protocol that scales efficiently to large groups and enjoys similar security guarantees remains largely open. The two existing proposals to date are ART (Cohn-Gordon et al., CCS18) and TreeKEM (IETF, The Messaging Layer Security Protocol, draft). TreeKEM is the currently considered candidate by the IETF MLS working group, but dynamic group operations (i.e. adding and removing users) can cause efficiency issues. In this paper we formalize and analyze a variant of TreeKEM which we term Tainted TreeKEM (TTKEM for short). The basic idea underlying TTKEM was suggested by Millican (MLS mailing list, February 2018). This version is more efficient than TreeKEM for some natural distributions of group operations, we quantify this through simulations.Our second contribution is two security proofs for TTKEM which establish post compromise and forward secrecy even against adaptive attackers. The security loss (to the underlying PKE) in the Random Oracle Model is a polynomial factor, and a quasipolynomial one in the Standard Model. Our proofs can be adapted to TreeKEM as well. Before our work no security proof for any TreeKEM-like protocol establishing tight security against an adversary who can adaptively choose the sequence of operations was known. We also are the first to prove (or even formalize) active security where the server can arbitrarily deviate from the protocol specification. Proving fully active security – where also the users can arbitrarily deviate – remains open.},
  author       = {Klein, Karen and Pascual Perez, Guillermo and Walter, Michael and Kamath Hosdurg, Chethan and Capretto, Margarita and Cueto Noval, Miguel and Markov, Ilia and Yeo, Michelle X and Alwen, Joel F and Pietrzak, Krzysztof Z},
  booktitle    = {2021 IEEE Symposium on Security and Privacy },
  location     = {San Francisco, CA, United States},
  pages        = {268--284},
  publisher    = {IEEE},
  title        = {{Keep the dirt: tainted TreeKEM, adaptively and actively secure continuous group key agreement}},
  doi          = {10.1109/sp40001.2021.00035},
  year         = {2021},
}

@article{8602,
  abstract     = {Collective cell migration offers a rich field of study for non-equilibrium physics and cellular biology, revealing phenomena such as glassy dynamics, pattern formation and active turbulence. However, how mechanical and chemical signalling are integrated at the cellular level to give rise to such collective behaviours remains unclear. We address this by focusing on the highly conserved phenomenon of spatiotemporal waves of density and extracellular signal-regulated kinase (ERK) activation, which appear both in vitro and in vivo during collective cell migration and wound healing. First, we propose a biophysical theory, backed by mechanical and optogenetic perturbation experiments, showing that patterns can be quantitatively explained by a mechanochemical coupling between active cellular tensions and the mechanosensitive ERK pathway. Next, we demonstrate how this biophysical mechanism can robustly induce long-ranged order and migration in a desired orientation, and we determine the theoretically optimal wavelength and period for inducing maximal migration towards free edges, which fits well with experimentally observed dynamics. We thereby provide a bridge between the biophysical origin of spatiotemporal instabilities and the design principles of robust and efficient long-ranged migration.},
  author       = {Boocock, Daniel R and Hino, Naoya and Ruzickova, Natalia and Hirashima, Tsuyoshi and Hannezo, Edouard B},
  issn         = {1745-2481},
  journal      = {Nature Physics},
  pages        = {267--274},
  publisher    = {Springer Nature},
  title        = {{Theory of mechanochemical patterning and optimal migration in cell monolayers}},
  doi          = {10.1038/s41567-020-01037-7},
  volume       = {17},
  year         = {2021},
}

@article{9817,
  abstract     = {Elastic bending of initially flat slender elements allows the realization and economic fabrication of intriguing curved shapes. In this work, we derive an intuitive but rigorous geometric characterization of the design space of plane elastic rods with variable stiffness. It enables designers to determine which shapes are physically viable with active bending by visual inspection alone. Building on these insights, we propose a method for efficiently designing the geometry of a flat elastic rod that realizes a target equilibrium curve, which only requires solving a linear program. We implement this method in an interactive computational design tool that gives feedback about the feasibility of a design, and computes the geometry of the structural elements necessary to realize it within an instant. The tool also offers an iterative optimization routine that improves the fabricability of a model while modifying it as little as possible. In addition, we use our geometric characterization to derive an algorithm for analyzing and recovering the stability of elastic curves that would otherwise snap out of their unstable equilibrium shapes by buckling. We show the efficacy of our approach by designing and manufacturing several physical models that are assembled from flat elements.},
  author       = {Hafner, Christian and Bickel, Bernd},
  issn         = {1557-7368},
  journal      = {ACM Transactions on Graphics},
  keywords     = {Computing methodologies, shape modeling, modeling and simulation, theory of computation, computational geometry, mathematics of computing, mathematical optimization},
  location     = {Virtual},
  number       = {4},
  publisher    = {Association for Computing Machinery},
  title        = {{The design space of plane elastic curves}},
  doi          = {10.1145/3450626.3459800},
  volume       = {40},
  year         = {2021},
}

@article{8966,
  abstract     = {During development, a single cell is transformed into a highly complex organism through progressive cell division, specification and rearrangement. An important prerequisite for the emergence of patterns within the developing organism is to establish asymmetries at various scales, ranging from individual cells to the entire embryo, eventually giving rise to the different body structures. This becomes especially apparent during gastrulation, when the earliest major lineage restriction events lead to the formation of the different germ layers. Traditionally, the unfolding of the developmental program from symmetry breaking to germ layer formation has been studied by dissecting the contributions of different signaling pathways and cellular rearrangements in the in vivo context of intact embryos. Recent efforts, using the intrinsic capacity of embryonic stem cells to self-assemble and generate embryo-like structures de novo, have opened new avenues for understanding the many ways by which an embryo can be built and the influence of extrinsic factors therein. Here, we discuss and compare divergent and conserved strategies leading to germ layer formation in embryos as compared to in vitro systems, their upstream molecular cascades and the role of extrinsic factors in this process.},
  author       = {Schauer, Alexandra and Heisenberg, Carl-Philipp J},
  issn         = {0012-1606},
  journal      = {Developmental Biology},
  keywords     = {Developmental Biology, Cell Biology, Molecular Biology},
  pages        = {71--81},
  publisher    = {Elsevier},
  title        = {{Reassembling gastrulation}},
  doi          = {10.1016/j.ydbio.2020.12.014},
  volume       = {474},
  year         = {2021},
}

@article{9438,
  abstract     = {Rigorous investigation of synaptic transmission requires analysis of unitary synaptic events by simultaneous recording from presynaptic terminals and postsynaptic target neurons. However, this has been achieved at only a limited number of model synapses, including the squid giant synapse and the mammalian calyx of Held. Cortical presynaptic terminals have been largely inaccessible to direct presynaptic recording, due to their small size. Here, we describe a protocol for improved subcellular patch-clamp recording in rat and mouse brain slices, with the synapse in a largely intact environment. Slice preparation takes ~2 h, recording ~3 h and post hoc morphological analysis 2 d. Single presynaptic hippocampal mossy fiber terminals are stimulated minimally invasively in the bouton-attached configuration, in which the cytoplasmic content remains unperturbed, or in the whole-bouton configuration, in which the cytoplasmic composition can be precisely controlled. Paired pre–postsynaptic recordings can be integrated with biocytin labeling and morphological analysis, allowing correlative investigation of synapse structure and function. Paired recordings can be obtained from mossy fiber terminals in slices from both rats and mice, implying applicability to genetically modified synapses. Paired recordings can also be performed together with axon tract stimulation or optogenetic activation, allowing comparison of unitary and compound synaptic events in the same target cell. Finally, paired recordings can be combined with spontaneous event analysis, permitting collection of miniature events generated at a single identified synapse. In conclusion, the subcellular patch-clamp techniques detailed here should facilitate analysis of biophysics, plasticity and circuit function of cortical synapses in the mammalian central nervous system.},
  author       = {Vandael, David H and Okamoto, Yuji and Borges Merjane, Carolina and Vargas Barroso, Victor M and Suter, Benjamin and Jonas, Peter M},
  issn         = {1750-2799},
  journal      = {Nature Protocols},
  number       = {6},
  pages        = {2947–2967},
  publisher    = {Springer Nature},
  title        = {{Subcellular patch-clamp techniques for single-bouton stimulation and simultaneous pre- and postsynaptic recording at cortical synapses}},
  doi          = {10.1038/s41596-021-00526-0},
  volume       = {16},
  year         = {2021},
}

@article{7883,
  abstract     = {All vertebrates have a spinal cord with dimensions and shape specific to their species. Yet how species‐specific organ size and shape are achieved is a fundamental unresolved question in biology. The formation and sculpting of organs begins during embryonic development. As it develops, the spinal cord extends in anterior–posterior direction in synchrony with the overall growth of the body. The dorsoventral (DV) and apicobasal lengths of the spinal cord neuroepithelium also change, while at the same time a characteristic pattern of neural progenitor subtypes along the DV axis is established and elaborated. At the basis of these changes in tissue size and shape are biophysical determinants, such as the change in cell number, cell size and shape, and anisotropic tissue growth. These processes are controlled by global tissue‐scale regulators, such as morphogen signaling gradients as well as mechanical forces. Current challenges in the field are to uncover how these tissue‐scale regulatory mechanisms are translated to the cellular and molecular level, and how regulation of distinct cellular processes gives rise to an overall defined size. Addressing these questions will help not only to achieve a better understanding of how size is controlled, but also of how tissue size is coordinated with the specification of pattern.},
  author       = {Kuzmicz-Kowalska, Katarzyna and Kicheva, Anna},
  issn         = {1759-7692},
  journal      = {Wiley Interdisciplinary Reviews: Developmental Biology},
  publisher    = {Wiley},
  title        = {{Regulation of size and scale in vertebrate spinal cord development}},
  doi          = {10.1002/wdev.383},
  year         = {2021},
}

@article{9349,
  abstract     = {The way in which interactions between mechanics and biochemistry lead to the emergence of complex cell and tissue organization is an old question that has recently attracted renewed interest from biologists, physicists, mathematicians and computer scientists. Rapid advances in optical physics, microscopy and computational image analysis have greatly enhanced our ability to observe and quantify spatiotemporal patterns of signalling, force generation, deformation, and flow in living cells and tissues. Powerful new tools for genetic, biophysical and optogenetic manipulation are allowing us to perturb the underlying machinery that generates these patterns in increasingly sophisticated ways. Rapid advances in theory and computing have made it possible to construct predictive models that describe how cell and tissue organization and dynamics emerge from the local coupling of biochemistry and mechanics. Together, these advances have opened up a wealth of new opportunities to explore how mechanochemical patterning shapes organismal development. In this roadmap, we present a series of forward-looking case studies on mechanochemical patterning in development, written by scientists working at the interface between the physical and biological sciences, and covering a wide range of spatial and temporal scales, organisms, and modes of development. Together, these contributions highlight the many ways in which the dynamic coupling of mechanics and biochemistry shapes biological dynamics: from mechanoenzymes that sense force to tune their activity and motor output, to collectives of cells in tissues that flow and redistribute biochemical signals during development.},
  author       = {Lenne, Pierre François and Munro, Edwin and Heemskerk, Idse and Warmflash, Aryeh and Bocanegra, Laura and Kishi, Kasumi and Kicheva, Anna and Long, Yuchen and Fruleux, Antoine and Boudaoud, Arezki and Saunders, Timothy E. and Caldarelli, Paolo and Michaut, Arthur and Gros, Jerome and Maroudas-Sacks, Yonit and Keren, Kinneret and Hannezo, Edouard B and Gartner, Zev J. and Stormo, Benjamin and Gladfelter, Amy and Rodrigues, Alan and Shyer, Amy and Minc, Nicolas and Maître, Jean Léon and Di Talia, Stefano and Khamaisi, Bassma and Sprinzak, David and Tlili, Sham},
  issn         = {1478-3975},
  journal      = {Physical biology},
  number       = {4},
  publisher    = {IOP Publishing},
  title        = {{Roadmap for the multiscale coupling of biochemical and mechanical signals during development}},
  doi          = {10.1088/1478-3975/abd0db},
  volume       = {18},
  year         = {2021},
}

@article{9250,
  abstract     = {Aprotic alkali metal–O2 batteries face two major obstacles to their chemistry occurring efficiently, the insulating nature of the formed alkali superoxides/peroxides and parasitic reactions that are caused by the highly reactive singlet oxygen (1O2). Redox mediators are recognized to be key for improving rechargeability. However, it is unclear how they affect 1O2 formation, which hinders strategies for their improvement. Here we clarify the mechanism of mediated peroxide and superoxide oxidation and thus explain how redox mediators either enhance or suppress 1O2 formation. We show that charging commences with peroxide oxidation to a superoxide intermediate and that redox potentials above ~3.5 V versus Li/Li+ drive 1O2 evolution from superoxide oxidation, while disproportionation always generates some 1O2. We find that 1O2 suppression requires oxidation to be faster than the generation of 1O2 from disproportionation. Oxidation rates decrease with growing driving force following Marcus inverted-region behaviour, establishing a region of maximum rate.},
  author       = {Petit, Yann K. and Mourad, Eléonore and Prehal, Christian and Leypold, Christian and Windischbacher, Andreas and Mijailovic, Daniel and Slugovc, Christian and Borisov, Sergey M. and Zojer, Egbert and Brutti, Sergio and Fontaine, Olivier and Freunberger, Stefan Alexander},
  issn         = {1755-4349},
  journal      = {Nature Chemistry},
  keywords     = {General Chemistry, General Chemical Engineering},
  number       = {5},
  pages        = {465--471},
  publisher    = {Springer Nature},
  title        = {{Mechanism of mediated alkali peroxide oxidation and triplet versus singlet oxygen formation}},
  doi          = {10.1038/s41557-021-00643-z},
  volume       = {13},
  year         = {2021},
}

@article{9428,
  abstract     = {Thermalization is the inevitable fate of many complex quantum systems, whose dynamics allow them to fully explore the vast configuration space regardless of the initial state---the behaviour known as quantum ergodicity. In a quest for experimental realizations of coherent long-time dynamics, efforts have focused on ergodicity-breaking mechanisms, such as integrability and localization. The recent discovery of persistent revivals in quantum simulators based on Rydberg atoms have pointed to the existence of a new type of behaviour where the system rapidly relaxes for most initial conditions, while certain initial states give rise to non-ergodic dynamics. This collective effect has been named ”quantum many-body scarring’by analogy with a related form of weak ergodicity breaking that occurs for a single particle inside a stadium billiard potential. In this Review, we provide a pedagogical introduction to quantum many-body scars and highlight the emerging connections with the semiclassical quantization of many-body systems. We discuss the relation between scars and more general routes towards weak violations of ergodicity due to embedded algebras and non-thermal eigenstates, and highlight possible applications of scars in quantum technology.},
  author       = {Serbyn, Maksym and Abanin, Dmitry A. and Papić, Zlatko},
  issn         = {1745-2481},
  journal      = {Nature Physics},
  number       = {6},
  pages        = {675–685},
  publisher    = {Nature Research},
  title        = {{Quantum many-body scars and weak breaking of ergodicity}},
  doi          = {10.1038/s41567-021-01230-2},
  volume       = {17},
  year         = {2021},
}

@phdthesis{9397,
  abstract     = {Accumulation of interstitial fluid (IF) between embryonic cells is a common phenomenon in vertebrate embryogenesis. Unlike other model systems, where these accumulations coalesce into a large central cavity – the blastocoel, in zebrafish, IF is more uniformly distributed between the deep cells (DC) before the onset of gastrulation. This is likely due to the presence of a large extraembryonic structure – the yolk cell (YC) at the position where the blastocoel typically forms in other model organisms. IF has long been speculated to play a role in tissue morphogenesis during embryogenesis, but direct evidence supporting such function is still sparse. Here we show that the relocalization of IF to the interface between the YC and DC/epiblast is critical for axial mesendoderm (ME) cell protrusion formation and migration along this interface, a key process in embryonic axis formation. We further demonstrate that axial ME cell migration and IF relocalization engage in a positive feedback loop, where axial ME migration triggers IF accumulation ahead of the advancing axial ME tissue by mechanically compressing the overlying epiblast cell layer. Upon compression, locally induced flow relocalizes the IF through the porous epiblast tissue resulting in an IF accumulation ahead of the leading axial ME. This IF accumulation, in turn, promotes cell protrusion formation and migration of the leading axial ME cells, thereby facilitating axial ME extension. Our findings reveal a central role of dynamic IF relocalization in orchestrating germ layer morphogenesis during gastrulation.},
  author       = {Huljev, Karla},
  issn         = {2663-337X},
  pages        = {101},
  publisher    = {Institute of Science and Technology Austria},
  title        = {{Coordinated spatiotemporal reorganization of interstitial fluid is required for axial mesendoderm migration in zebrafish gastrulation}},
  doi          = {10.15479/at:ista:9397},
  year         = {2021},
}

@phdthesis{9992,
  abstract     = {Blood – this is what animals use to heal wounds fast and efficient. Plants do not have blood circulation and their cells cannot move. However, plants have evolved remarkable capacities to regenerate tissues and organs preventing further damage. In my PhD research, I studied the wound healing in the Arabidopsis root. I used a UV laser to ablate single cells in the root tip and observed the consequent wound healing. Interestingly, the inner adjacent cells induced a
division plane switch and subsequently adopted the cell type of the killed cell to replace it. We termed this form of wound healing “restorative divisions”. This initial observation triggered the questions of my PhD studies: How and why do cells orient their division planes, how do they feel the wound and why does this happen only in inner adjacent cells.
For answering these questions, I used a quite simple experimental setup: 5 day - old seedlings were stained with propidium iodide to visualize cell walls and dead cells; ablation was carried out using a special laser cutter and a confocal microscope. Adaptation of the novel vertical microscope system made it possible to observe wounds in real time. This revealed that restorative divisions occur at increased frequency compared to normal divisions. Additionally,
the major plant hormone auxin accumulates in wound adjacent cells and drives the expression of the wound-stress responsive transcription factor ERF115. Using this as a marker gene for wound responses, we found that an important part of wound signalling is the sensing of the collapse of the ablated cell. The collapse causes a radical pressure drop, which results in strong tissue deformations. These deformations manifest in an invasion of the now free spot specifically by the inner adjacent cells within seconds, probably because of higher pressure of the inner tissues. Long-term imaging revealed that those deformed cells continuously expand towards the wound hole and that this is crucial for the restorative division. These wound-expanding cells exhibit an abnormal, biphasic polarity of microtubule arrays
before the division. Experiments inhibiting cell expansion suggest that it is the biphasic stretching that induces those MT arrays. Adapting the micromanipulator aspiration system from animal scientists at our institute confirmed the hypothesis that stretching influences microtubule stability. In conclusion, this shows that microtubules react to tissue deformation
and this facilitates the observed division plane switch. This puts mechanical cues and tensions at the most prominent position for explaining the growth and wound healing properties of plants. Hence, it shines light onto the importance of understanding mechanical signal transduction. },
  author       = {Hörmayer, Lukas},
  issn         = {2663-337X},
  pages        = {168},
  publisher    = {Institute of Science and Technology Austria},
  title        = {{Wound healing in the Arabidopsis root meristem}},
  doi          = {10.15479/at:ista:9992},
  year         = {2021},
}

@phdthesis{9728,
  abstract     = {Most real-world flows are multiphase, yet we know little about them compared to their single-phase counterparts. Multiphase flows are more difficult to investigate as their dynamics occur in large parameter space and involve complex phenomena such as preferential concentration, turbulence modulation, non-Newtonian rheology, etc. Over the last few decades, experiments in particle-laden flows have taken a back seat in favour of ever-improving computational resources. However, computers are still not powerful enough to simulate a real-world fluid with millions of finite-size particles. Experiments are essential not only because they offer a reliable way to investigate real-world multiphase flows but also because they serve to validate numerical studies and steer the research in a relevant direction. In this work, we have experimentally investigated particle-laden flows in pipes, and in particular, examined the effect of particles on the laminar-turbulent transition and the drag scaling in turbulent flows.

For particle-laden pipe flows, an earlier study [Matas et al., 2003] reported how the sub-critical (i.e., hysteretic) transition that occurs via localised turbulent structures called puffs is affected by the addition of particles. In this study, in addition to this known transition, we found a super-critical transition to a globally fluctuating state with increasing particle concentration. At the same time, the Newtonian-type transition via puffs is delayed to larger Reynolds numbers. At an even higher concentration, only the globally fluctuating state is found. The dynamics of particle-laden flows are hence determined by two competing instabilities that give rise to three flow regimes: Newtonian-type turbulence at low, a particle-induced globally fluctuating state at high, and a coexistence state at intermediate concentrations.

The effect of particles on turbulent drag is ambiguous, with studies reporting drag reduction, no net change, and even drag increase. The ambiguity arises because, in addition to particle concentration, particle shape, size, and density also affect the net drag. Even similar particles might affect the flow dissimilarly in different Reynolds number and concentration ranges. In the present study, we explored a wide range of both Reynolds number and concentration, using spherical as well as cylindrical particles. We found that the spherical particles do not reduce drag while the cylindrical particles are drag-reducing within a specific Reynolds number interval. The interval strongly depends on the particle concentration and the relative size of the pipe and particles. Within this interval, the magnitude of drag reduction reaches a maximum. These drag reduction maxima appear to fall onto a distinct power-law curve irrespective of the pipe diameter and particle concentration, and this curve can be considered as the maximum drag reduction asymptote for a given fibre shape. Such an asymptote is well known for polymeric flows but had not been identified for particle-laden flows prior to this work.},
  author       = {Agrawal, Nishchal},
  issn         = {2663-337X},
  keywords     = {Drag Reduction, Transition to Turbulence, Multiphase Flows, particle Laden Flows, Complex Flows, Experiments, Fluid Dynamics},
  pages        = {118},
  publisher    = {Institute of Science and Technology Austria},
  title        = {{Transition to turbulence and drag reduction in particle-laden pipe flows}},
  doi          = {10.15479/at:ista:9728},
  year         = {2021},
}

@unpublished{10077,
  abstract     = {Although much is known about how single neurons in the hippocampus represent an animal’s position, how cell-cell interactions contribute to spatial coding remains poorly understood. Using a novel statistical estimator and theoretical modeling, both developed in the framework of maximum entropy models, we reveal highly structured cell-to-cell interactions whose statistics depend on familiar vs. novel environment. In both conditions the circuit interactions optimize the encoding of spatial information, but for regimes that differ in the signal-to-noise ratio of their spatial inputs. Moreover, the topology of the interactions facilitates linear decodability, making the information easy to read out by downstream circuits. These findings suggest that the efficient coding hypothesis is not applicable only to individual neuron properties in the sensory periphery, but also to neural interactions in the central brain.},
  author       = {Nardin, Michele and Csicsvari, Jozsef L and Tkačik, Gašper and Savin, Cristina},
  booktitle    = {bioRxiv},
  title        = {{The structure of hippocampal CA1 interactions optimizes spatial coding across experience}},
  doi          = {10.1101/2021.09.28.460602},
  year         = {2021},
}