Focus on:
All days
4 Apr 2022
5 Apr 2022
6 Apr 2022
7 Apr 2022
8 Apr 2022
9 Apr 2022
10 Apr 2022
11 Apr 2022
12 Apr 2022
13 Apr 2022
14 Apr 2022
15 Apr 2022
16 Apr 2022
17 Apr 2022
18 Apr 2022
19 Apr 2022
20 Apr 2022
21 Apr 2022
22 Apr 2022
23 Apr 2022
24 Apr 2022
25 Apr 2022
26 Apr 2022
27 Apr 2022
28 Apr 2022
29 Apr 2022
30 Apr 2022
1 May 2022
2 May 2022
3 May 2022
4 May 2022
5 May 2022
6 May 2022
7 May 2022
8 May 2022
9 May 2022
10 May 2022
11 May 2022
12 May 2022
13 May 2022
14 May 2022
15 May 2022
16 May 2022
17 May 2022
18 May 2022
19 May 2022
20 May 2022
21 May 2022
22 May 2022
23 May 2022
24 May 2022
25 May 2022
26 May 2022
27 May 2022
28 May 2022
29 May 2022
30 May 2022
31 May 2022
1 Jun 2022
2 Jun 2022
3 Jun 2022
4 Jun 2022
5 Jun 2022
6 Jun 2022
7 Jun 2022
8 Jun 2022
9 Jun 2022
10 Jun 2022
11 Jun 2022
12 Jun 2022
13 Jun 2022
14 Jun 2022
15 Jun 2022
16 Jun 2022
17 Jun 2022
18 Jun 2022
19 Jun 2022
20 Jun 2022
21 Jun 2022
22 Jun 2022
23 Jun 2022
24 Jun 2022
25 Jun 2022
26 Jun 2022
27 Jun 2022
28 Jun 2022
29 Jun 2022
30 Jun 2022
1 Jul 2022
2 Jul 2022
3 Jul 2022
4 Jul 2022
5 Jul 2022
6 Jul 2022
7 Jul 2022
8 Jul 2022
9 Jul 2022
10 Jul 2022
11 Jul 2022
12 Jul 2022
13 Jul 2022
14 Jul 2022
15 Jul 2022
16 Jul 2022
17 Jul 2022
18 Jul 2022
19 Jul 2022
20 Jul 2022
21 Jul 2022
22 Jul 2022
23 Jul 2022
24 Jul 2022
25 Jul 2022
26 Jul 2022
27 Jul 2022
28 Jul 2022
29 Jul 2022
30 Jul 2022
31 Jul 2022
1 Aug 2022
2 Aug 2022
3 Aug 2022
4 Aug 2022
5 Aug 2022
6 Aug 2022
7 Aug 2022
8 Aug 2022
9 Aug 2022
10 Aug 2022
11 Aug 2022
12 Aug 2022
13 Aug 2022
14 Aug 2022
15 Aug 2022
16 Aug 2022
17 Aug 2022
18 Aug 2022
19 Aug 2022
20 Aug 2022
21 Aug 2022
22 Aug 2022
23 Aug 2022
24 Aug 2022
25 Aug 2022
26 Aug 2022
27 Aug 2022
28 Aug 2022
29 Aug 2022
30 Aug 2022
31 Aug 2022
1 Sept 2022
2 Sept 2022
3 Sept 2022
4 Sept 2022
5 Sept 2022
6 Sept 2022
7 Sept 2022
8 Sept 2022
9 Sept 2022
10 Sept 2022
11 Sept 2022
12 Sept 2022
13 Sept 2022
14 Sept 2022
15 Sept 2022
16 Sept 2022
17 Sept 2022
18 Sept 2022
19 Sept 2022
20 Sept 2022
21 Sept 2022
22 Sept 2022
23 Sept 2022
24 Sept 2022
25 Sept 2022
26 Sept 2022
27 Sept 2022
28 Sept 2022
29 Sept 2022
30 Sept 2022
1 Oct 2022
2 Oct 2022
3 Oct 2022
4 Oct 2022
5 Oct 2022
6 Oct 2022
7 Oct 2022
8 Oct 2022
9 Oct 2022
10 Oct 2022
11 Oct 2022
12 Oct 2022
13 Oct 2022
14 Oct 2022
15 Oct 2022
16 Oct 2022
17 Oct 2022
18 Oct 2022
19 Oct 2022
20 Oct 2022
21 Oct 2022
22 Oct 2022
23 Oct 2022
24 Oct 2022
25 Oct 2022
26 Oct 2022
27 Oct 2022
28 Oct 2022
29 Oct 2022
30 Oct 2022
31 Oct 2022
1 Nov 2022
2 Nov 2022
3 Nov 2022
4 Nov 2022
5 Nov 2022
6 Nov 2022
7 Nov 2022
8 Nov 2022
9 Nov 2022
10 Nov 2022
11 Nov 2022
12 Nov 2022
13 Nov 2022
14 Nov 2022
15 Nov 2022
16 Nov 2022
17 Nov 2022
18 Nov 2022
19 Nov 2022
20 Nov 2022
21 Nov 2022
22 Nov 2022
23 Nov 2022
24 Nov 2022
25 Nov 2022
26 Nov 2022
27 Nov 2022
28 Nov 2022
29 Nov 2022
30 Nov 2022
1 Dec 2022
2 Dec 2022
3 Dec 2022
4 Dec 2022
5 Dec 2022
6 Dec 2022
7 Dec 2022
8 Dec 2022
9 Dec 2022
10 Dec 2022
11 Dec 2022
12 Dec 2022
13 Dec 2022
14 Dec 2022
15 Dec 2022
16 Dec 2022
17 Dec 2022
18 Dec 2022
19 Dec 2022
20 Dec 2022
21 Dec 2022
22 Dec 2022
23 Dec 2022
24 Dec 2022
25 Dec 2022
26 Dec 2022
27 Dec 2022
28 Dec 2022
29 Dec 2022
30 Dec 2022
31 Dec 2022
Indico style
Indico style - inline minutes
Indico style - numbered
Indico style - numbered + minutes
Indico Weeks View
Choose Timezone
Use the event/category timezone
Specify a timezone
Africa/Abidjan
Africa/Accra
Africa/Addis_Ababa
Africa/Algiers
Africa/Asmara
Africa/Bamako
Africa/Bangui
Africa/Banjul
Africa/Bissau
Africa/Blantyre
Africa/Brazzaville
Africa/Bujumbura
Africa/Cairo
Africa/Casablanca
Africa/Ceuta
Africa/Conakry
Africa/Dakar
Africa/Dar_es_Salaam
Africa/Djibouti
Africa/Douala
Africa/El_Aaiun
Africa/Freetown
Africa/Gaborone
Africa/Harare
Africa/Johannesburg
Africa/Juba
Africa/Kampala
Africa/Khartoum
Africa/Kigali
Africa/Kinshasa
Africa/Lagos
Africa/Libreville
Africa/Lome
Africa/Luanda
Africa/Lubumbashi
Africa/Lusaka
Africa/Malabo
Africa/Maputo
Africa/Maseru
Africa/Mbabane
Africa/Mogadishu
Africa/Monrovia
Africa/Nairobi
Africa/Ndjamena
Africa/Niamey
Africa/Nouakchott
Africa/Ouagadougou
Africa/Porto-Novo
Africa/Sao_Tome
Africa/Tripoli
Africa/Tunis
Africa/Windhoek
America/Adak
America/Anchorage
America/Anguilla
America/Antigua
America/Araguaina
America/Argentina/Buenos_Aires
America/Argentina/Catamarca
America/Argentina/Cordoba
America/Argentina/Jujuy
America/Argentina/La_Rioja
America/Argentina/Mendoza
America/Argentina/Rio_Gallegos
America/Argentina/Salta
America/Argentina/San_Juan
America/Argentina/San_Luis
America/Argentina/Tucuman
America/Argentina/Ushuaia
America/Aruba
America/Asuncion
America/Atikokan
America/Bahia
America/Bahia_Banderas
America/Barbados
America/Belem
America/Belize
America/Blanc-Sablon
America/Boa_Vista
America/Bogota
America/Boise
America/Cambridge_Bay
America/Campo_Grande
America/Cancun
America/Caracas
America/Cayenne
America/Cayman
America/Chicago
America/Chihuahua
America/Ciudad_Juarez
America/Costa_Rica
America/Creston
America/Cuiaba
America/Curacao
America/Danmarkshavn
America/Dawson
America/Dawson_Creek
America/Denver
America/Detroit
America/Dominica
America/Edmonton
America/Eirunepe
America/El_Salvador
America/Fort_Nelson
America/Fortaleza
America/Glace_Bay
America/Goose_Bay
America/Grand_Turk
America/Grenada
America/Guadeloupe
America/Guatemala
America/Guayaquil
America/Guyana
America/Halifax
America/Havana
America/Hermosillo
America/Indiana/Indianapolis
America/Indiana/Knox
America/Indiana/Marengo
America/Indiana/Petersburg
America/Indiana/Tell_City
America/Indiana/Vevay
America/Indiana/Vincennes
America/Indiana/Winamac
America/Inuvik
America/Iqaluit
America/Jamaica
America/Juneau
America/Kentucky/Louisville
America/Kentucky/Monticello
America/Kralendijk
America/La_Paz
America/Lima
America/Los_Angeles
America/Lower_Princes
America/Maceio
America/Managua
America/Manaus
America/Marigot
America/Martinique
America/Matamoros
America/Mazatlan
America/Menominee
America/Merida
America/Metlakatla
America/Mexico_City
America/Miquelon
America/Moncton
America/Monterrey
America/Montevideo
America/Montserrat
America/Nassau
America/New_York
America/Nome
America/Noronha
America/North_Dakota/Beulah
America/North_Dakota/Center
America/North_Dakota/New_Salem
America/Nuuk
America/Ojinaga
America/Panama
America/Paramaribo
America/Phoenix
America/Port-au-Prince
America/Port_of_Spain
America/Porto_Velho
America/Puerto_Rico
America/Punta_Arenas
America/Rankin_Inlet
America/Recife
America/Regina
America/Resolute
America/Rio_Branco
America/Santarem
America/Santiago
America/Santo_Domingo
America/Sao_Paulo
America/Scoresbysund
America/Sitka
America/St_Barthelemy
America/St_Johns
America/St_Kitts
America/St_Lucia
America/St_Thomas
America/St_Vincent
America/Swift_Current
America/Tegucigalpa
America/Thule
America/Tijuana
America/Toronto
America/Tortola
America/Vancouver
America/Whitehorse
America/Winnipeg
America/Yakutat
Antarctica/Casey
Antarctica/Davis
Antarctica/DumontDUrville
Antarctica/Macquarie
Antarctica/Mawson
Antarctica/McMurdo
Antarctica/Palmer
Antarctica/Rothera
Antarctica/Syowa
Antarctica/Troll
Antarctica/Vostok
Arctic/Longyearbyen
Asia/Aden
Asia/Almaty
Asia/Amman
Asia/Anadyr
Asia/Aqtau
Asia/Aqtobe
Asia/Ashgabat
Asia/Atyrau
Asia/Baghdad
Asia/Bahrain
Asia/Baku
Asia/Bangkok
Asia/Barnaul
Asia/Beirut
Asia/Bishkek
Asia/Brunei
Asia/Chita
Asia/Choibalsan
Asia/Colombo
Asia/Damascus
Asia/Dhaka
Asia/Dili
Asia/Dubai
Asia/Dushanbe
Asia/Famagusta
Asia/Gaza
Asia/Hebron
Asia/Ho_Chi_Minh
Asia/Hong_Kong
Asia/Hovd
Asia/Irkutsk
Asia/Jakarta
Asia/Jayapura
Asia/Jerusalem
Asia/Kabul
Asia/Kamchatka
Asia/Karachi
Asia/Kathmandu
Asia/Khandyga
Asia/Kolkata
Asia/Krasnoyarsk
Asia/Kuala_Lumpur
Asia/Kuching
Asia/Kuwait
Asia/Macau
Asia/Magadan
Asia/Makassar
Asia/Manila
Asia/Muscat
Asia/Nicosia
Asia/Novokuznetsk
Asia/Novosibirsk
Asia/Omsk
Asia/Oral
Asia/Phnom_Penh
Asia/Pontianak
Asia/Pyongyang
Asia/Qatar
Asia/Qostanay
Asia/Qyzylorda
Asia/Riyadh
Asia/Sakhalin
Asia/Samarkand
Asia/Seoul
Asia/Shanghai
Asia/Singapore
Asia/Srednekolymsk
Asia/Taipei
Asia/Tashkent
Asia/Tbilisi
Asia/Tehran
Asia/Thimphu
Asia/Tokyo
Asia/Tomsk
Asia/Ulaanbaatar
Asia/Urumqi
Asia/Ust-Nera
Asia/Vientiane
Asia/Vladivostok
Asia/Yakutsk
Asia/Yangon
Asia/Yekaterinburg
Asia/Yerevan
Atlantic/Azores
Atlantic/Bermuda
Atlantic/Canary
Atlantic/Cape_Verde
Atlantic/Faroe
Atlantic/Madeira
Atlantic/Reykjavik
Atlantic/South_Georgia
Atlantic/St_Helena
Atlantic/Stanley
Australia/Adelaide
Australia/Brisbane
Australia/Broken_Hill
Australia/Darwin
Australia/Eucla
Australia/Hobart
Australia/Lindeman
Australia/Lord_Howe
Australia/Melbourne
Australia/Perth
Australia/Sydney
Canada/Atlantic
Canada/Central
Canada/Eastern
Canada/Mountain
Canada/Newfoundland
Canada/Pacific
Europe/Amsterdam
Europe/Andorra
Europe/Astrakhan
Europe/Athens
Europe/Belgrade
Europe/Berlin
Europe/Bratislava
Europe/Brussels
Europe/Bucharest
Europe/Budapest
Europe/Busingen
Europe/Chisinau
Europe/Copenhagen
Europe/Dublin
Europe/Gibraltar
Europe/Guernsey
Europe/Helsinki
Europe/Isle_of_Man
Europe/Istanbul
Europe/Jersey
Europe/Kaliningrad
Europe/Kirov
Europe/Kyiv
Europe/Lisbon
Europe/Ljubljana
Europe/London
Europe/Luxembourg
Europe/Madrid
Europe/Malta
Europe/Mariehamn
Europe/Minsk
Europe/Monaco
Europe/Moscow
Europe/Oslo
Europe/Paris
Europe/Podgorica
Europe/Prague
Europe/Riga
Europe/Rome
Europe/Samara
Europe/San_Marino
Europe/Sarajevo
Europe/Saratov
Europe/Simferopol
Europe/Skopje
Europe/Sofia
Europe/Stockholm
Europe/Tallinn
Europe/Tirane
Europe/Ulyanovsk
Europe/Vaduz
Europe/Vatican
Europe/Vienna
Europe/Vilnius
Europe/Volgograd
Europe/Warsaw
Europe/Zagreb
Europe/Zurich
GMT
Indian/Antananarivo
Indian/Chagos
Indian/Christmas
Indian/Cocos
Indian/Comoro
Indian/Kerguelen
Indian/Mahe
Indian/Maldives
Indian/Mauritius
Indian/Mayotte
Indian/Reunion
Pacific/Apia
Pacific/Auckland
Pacific/Bougainville
Pacific/Chatham
Pacific/Chuuk
Pacific/Easter
Pacific/Efate
Pacific/Fakaofo
Pacific/Fiji
Pacific/Funafuti
Pacific/Galapagos
Pacific/Gambier
Pacific/Guadalcanal
Pacific/Guam
Pacific/Honolulu
Pacific/Kanton
Pacific/Kiritimati
Pacific/Kosrae
Pacific/Kwajalein
Pacific/Majuro
Pacific/Marquesas
Pacific/Midway
Pacific/Nauru
Pacific/Niue
Pacific/Norfolk
Pacific/Noumea
Pacific/Pago_Pago
Pacific/Palau
Pacific/Pitcairn
Pacific/Pohnpei
Pacific/Port_Moresby
Pacific/Rarotonga
Pacific/Saipan
Pacific/Tahiti
Pacific/Tarawa
Pacific/Tongatapu
Pacific/Wake
Pacific/Wallis
US/Alaska
US/Arizona
US/Central
US/Eastern
US/Hawaii
US/Mountain
US/Pacific
UTC
Save
Europe/Rome
English (United Kingdom)
Deutsch (Deutschland)
English (United Kingdom)
English (United States)
Español (España)
Français (France)
Italiano (Italia)
Polski (Polska)
Português (Brasil)
Türkçe (Türkiye)
Čeština (Česko)
Монгол (Монгол)
Українська (Україна)
中文 (中国)
Login
Theory Lectures by Young Researchers - ThLYR 2022
from
Monday, 4 April 2022 (09:00)
to
Saturday, 31 December 2022 (18:00)
Monday, 4 April 2022
10:00
An Introduction to Quantum Computing for Lattice Quantum Field Theory - I
-
Giuseppe Clemente
(
DESY Zeuthen
)
An Introduction to Quantum Computing for Lattice Quantum Field Theory - I
Giuseppe Clemente
(
DESY Zeuthen
)
10:00 - 12:00
Room: Zoom Room
Classical state-of-the-art numerical techniques have pushed the measurements of quantities of interest for Lattice Quantum Field Theories to unprecedented degrees of accuracy. However, these techniques have limitations and some problems are still difficult to investigate. As Feynman noticed decades ago, quantum computation presents itself as a more natural setting to study the physics of quantum systems; as quantum computers and quantum technologies are improving from year to year, quantum computation techniques are becoming increasingly important tools in the theoretical physicist's toolkit. In these lectures I will first give a broad introduction to the fundamentals of quantum computing, discussing some of the main algorithms and applications. Then, I will discuss some of the most promising quantum computing techniques for solving Lattice Quantum Field Theory problems in regimes where classical methods cannot be applied or are especially expensive from the computational point of view.
Tuesday, 5 April 2022
10:00
An Introduction to Quantum Computing for Lattice Quantum Field Theory - II
-
Giuseppe Clemente
(
DESY Zeuthen
)
An Introduction to Quantum Computing for Lattice Quantum Field Theory - II
Giuseppe Clemente
(
DESY Zeuthen
)
10:00 - 12:00
Room: Zoom Room
Classical state-of-the-art numerical techniques have pushed the measurements of quantities of interest for Lattice Quantum Field Theories to unprecedented degrees of accuracy. However, these techniques have limitations and some problems are still difficult to investigate. As Feynman noticed decades ago, quantum computation presents itself as a more natural setting to study the physics of quantum systems; as quantum computers and quantum technologies are improving from year to year, quantum computation techniques are becoming increasingly important tools in the theoretical physicist's toolkit. In these lectures I will first give a broad introduction to the fundamentals of quantum computing, discussing some of the main algorithms and applications. Then, I will discuss some of the most promising quantum computing techniques for solving Lattice Quantum Field Theory problems in regimes where classical methods cannot be applied or are especially expensive from the computational point of view.
Wednesday, 6 April 2022
Thursday, 7 April 2022
Friday, 8 April 2022
Saturday, 9 April 2022
Sunday, 10 April 2022
Monday, 11 April 2022
Tuesday, 12 April 2022
Wednesday, 13 April 2022
Thursday, 14 April 2022
Friday, 15 April 2022
Saturday, 16 April 2022
Sunday, 17 April 2022
Monday, 18 April 2022
Tuesday, 19 April 2022
Wednesday, 20 April 2022
Thursday, 21 April 2022
Friday, 22 April 2022
Saturday, 23 April 2022
Sunday, 24 April 2022
Monday, 25 April 2022
Tuesday, 26 April 2022
14:30
Techniques for statistical analysis of cosmological data - (Lecture 1 of 2)
-
Fabrizio Renzi
(
Leiden University
)
Techniques for statistical analysis of cosmological data - (Lecture 1 of 2)
Fabrizio Renzi
(
Leiden University
)
14:30 - 16:30
Room: Zoom Room
Analyzing data is an interplay between modeling physical theories and using complex statistical inference to extract unbiased information from the data themselves. In the era of precision cosmology, data analysis has become a key tool for the falsification of cosmological theories and for the quest of finding new physical effects not predicted by our current modelization of the Universe. Inevitably, many biases are introduced, willingly or not, in the procedure of extracting information from data since our theories are incomplete and our statistical inference is not perfect. Such biases could lead to wrong physical conclusions and particular care is required in deriving answers that are as free as possible from those biases. In this series of two lectures, I will give an introduction to Monte Carlo Markov Chain (MCMC) and Machine Learning (ML) techniques for the inference of cosmological parameters. I will discuss their advantages and disadvantages and show how they can be used to gain accurate information about our Universe. The first lecture will be dedicated to introducing the building blocks of statistical inference. Starting from the simplest example of fitting a linear model to data, I will introduce the main concepts behind the construction of MCMC and ML methods and show how to use them with real examples. The second lecture will be dedicated to learning to use these methodologies to analyze real cosmological data and derive constraints on cosmological parameters. In particular, I will show the use of low-redshift (late-time) cosmological data to bound the Hubble parameter and discuss the results in view of the current literature on the Hubble tension.
Wednesday, 27 April 2022
10:30
Techniques for statistical analysis of cosmological data - (Lecture 2 of 2)
-
Fabrizio Renzi
(
Leiden University
)
Techniques for statistical analysis of cosmological data - (Lecture 2 of 2)
Fabrizio Renzi
(
Leiden University
)
10:30 - 12:30
Room: Zoom Room
Analyzing data is an interplay between modeling physical theories and using complex statistical inference to extract unbiased information from the data themselves. In the era of precision cosmology, data analysis has become a key tool for the falsification of cosmological theories and for the quest of finding new physical effects not predicted by our current modelization of the Universe. Inevitably, many biases are introduced, willingly or not, in the procedure of extracting information from data since our theories are incomplete and our statistical inference is not perfect. Such biases could lead to wrong physical conclusions and particular care is required in deriving answers that are as free as possible from those biases. In this series of two lectures, I will give an introduction to Monte Carlo Markov Chain (MCMC) and Machine Learning (ML) techniques for the inference of cosmological parameters. I will discuss their advantages and disadvantages and show how they can be used to gain accurate information about our Universe. The first lecture will be dedicated to introducing the building blocks of statistical inference. Starting from the simplest example of fitting a linear model to data, I will introduce the main concepts behind the construction of MCMC and ML methods and show how to use them with real examples. The second lecture will be dedicated to learning to use these methodologies to analyze real cosmological data and derive constraints on cosmological parameters. In particular, I will show the use of low-redshift (late-time) cosmological data to bound the Hubble parameter and discuss the results in view of the current literature on the Hubble tension.
Thursday, 28 April 2022
Friday, 29 April 2022
Saturday, 30 April 2022
Sunday, 1 May 2022
Monday, 2 May 2022
Tuesday, 3 May 2022
Wednesday, 4 May 2022
Thursday, 5 May 2022
10:30
An introduction to tensor models: from random geometry to melonic CFTs - (Lecture 1 of 2)
-
Sabine Harribey
(
Ecole Polytechnique, CPHT and U. Heidelberg, ITP
)
An introduction to tensor models: from random geometry to melonic CFTs - (Lecture 1 of 2)
Sabine Harribey
(
Ecole Polytechnique, CPHT and U. Heidelberg, ITP
)
10:30 - 12:30
Room: Zoom Room
Tensor models are particularly interesting due to their melonic large-$N$ limit which is richer than the large-$N$ limit of vector models but simpler than the planar limit of matrix models. Tensor models were first introduced in zero dimension in the context of random geometry and quantum gravity. They were then extended to quantum mechanical models in one dimension as an alternative to the Sachdev-Ye-Kitaev model without disorder. Finally, they were generalized in higher dimensions as toy models for strongly-coupled QFTs. In this context, they give rise in the infrared to a new kind of conformal field theories analytically accessible, called melonic CFTs. In these lectures, after reviewing the large-$N$ expansion of matrix models, I will introduce tensor models and derive their melonic large-$N$ limit. In both cases, I will present some applications to random geometry and quantum gravity. The second part of the lectures will focus on melonic CFTs. In particular, I will review the bosonic long-range $O(N)^3$ model giving rise at large $N$ to a unitary CFT in the infrared.
Friday, 6 May 2022
10:30
An introduction to tensor models: from random geometry to melonic CFTs - (Lecture 2 of 2)
-
Sabine Harribey
(
Ecole Polytechnique, CPHT and U. Heidelberg, ITP
)
An introduction to tensor models: from random geometry to melonic CFTs - (Lecture 2 of 2)
Sabine Harribey
(
Ecole Polytechnique, CPHT and U. Heidelberg, ITP
)
10:30 - 12:30
Room: Zoom Room
Tensor models are particularly interesting due to their melonic large-$N$ limit which is richer than the large-$N$ limit of vector models but simpler than the planar limit of matrix models. Tensor models were first introduced in zero dimension in the context of random geometry and quantum gravity. They were then extended to quantum mechanical models in one dimension as an alternative to the Sachdev-Ye-Kitaev model without disorder. Finally, they were generalized in higher dimensions as toy models for strongly-coupled QFTs. In this context, they give rise in the infrared to a new kind of conformal field theories analytically accessible, called melonic CFTs. In these lectures, after reviewing the large-$N$ expansion of matrix models, I will introduce tensor models and derive their melonic large-$N$ limit. In both cases, I will present some applications to random geometry and quantum gravity. The second part of the lectures will focus on melonic CFTs. In particular, I will review the bosonic long-range $O(N)^3$ model giving rise at large $N$ to a unitary CFT in the infrared.
Saturday, 7 May 2022
Sunday, 8 May 2022
Monday, 9 May 2022
Tuesday, 10 May 2022
Wednesday, 11 May 2022
10:00
Modern Non-Perturbative Techniques in QFT - Lecture 1
-
Karateev Denis
(
University of Geneva
)
Modern Non-Perturbative Techniques in QFT - Lecture 1
Karateev Denis
(
University of Geneva
)
10:00 - 12:30
Room: Zoom Room
I will define quantum field theories (QFTs) Non-Perturbatively and discuss their observables. I will review modern techniques, such as the Conformal and S-matrix Bootstrap, which allow to bound the space of consistent QFTs and, in particular cases, even to compute some observables.
Thursday, 12 May 2022
10:00
Modern Non-Perturbative Techniques in QFT - Lecture 2
-
Karateev Denis
(
University of Geneva
)
Modern Non-Perturbative Techniques in QFT - Lecture 2
Karateev Denis
(
University of Geneva
)
10:00 - 12:30
Room: Zoom Room
I will define quantum field theories (QFTs) Non-Perturbatively and discuss their observables. I will review modern techniques, such as the Conformal and S-matrix Bootstrap, which allow to bound the space of consistent QFTs and, in particular cases, even to compute some observables.
Friday, 13 May 2022
Saturday, 14 May 2022
Sunday, 15 May 2022
Monday, 16 May 2022
Tuesday, 17 May 2022
Wednesday, 18 May 2022
Thursday, 19 May 2022
Friday, 20 May 2022
Saturday, 21 May 2022
Sunday, 22 May 2022
Monday, 23 May 2022
Tuesday, 24 May 2022
Wednesday, 25 May 2022
Thursday, 26 May 2022
Friday, 27 May 2022
Saturday, 28 May 2022
Sunday, 29 May 2022
Monday, 30 May 2022
Tuesday, 31 May 2022
11:00
Density functionals in nuclear systems
-
Chiranjib Mondal
(
Université de Caen Normandie
)
Density functionals in nuclear systems
Chiranjib Mondal
(
Université de Caen Normandie
)
11:00 - 13:00
Room: Zoom Room
In these two lectures, I will give a general overview of density functional theory (DFT) in nuclear systems. We will discuss the basic ingredients of the theory in terms of similarities and (of course) differences with an electronic system. We will discuss further, with an illustrating example, how to find the ground state properties of a simple nucleus and properties of infinite nuclear matter. We will end the discussion with constructing an energy density functional (EDF) which is cost effective, agnostic yet informed by nuclear properties, suitable for astrophysical calculations.
Wednesday, 1 June 2022
Thursday, 2 June 2022
Friday, 3 June 2022
11:00
Density functionals in nuclear systems
-
Chiranjib Mondal
(
Université de Caen Normandie
)
Density functionals in nuclear systems
Chiranjib Mondal
(
Université de Caen Normandie
)
11:00 - 13:00
Room: Zoom Room
In these two lectures, I will give a general overview of density functional theory (DFT) in nuclear systems. We will discuss the basic ingredients of the theory in terms of similarities and (of course) differences with an electronic system. We will discuss further, with an illustrating example, how to find the ground state properties of a simple nucleus and properties of infinite nuclear matter. We will end the discussion with constructing an energy density functional (EDF) which is cost effective, agnostic yet informed by nuclear properties, suitable for astrophysical calculations.
Saturday, 4 June 2022
Sunday, 5 June 2022
Monday, 6 June 2022
Tuesday, 7 June 2022
Wednesday, 8 June 2022
Thursday, 9 June 2022
Friday, 10 June 2022
Saturday, 11 June 2022
Sunday, 12 June 2022
Monday, 13 June 2022
Tuesday, 14 June 2022
Wednesday, 15 June 2022
08:00
A Graph-Theoretic Approach to Free-Fermion Solvability
-
Adrian Chapman
(
Oxford
)
A Graph-Theoretic Approach to Free-Fermion Solvability
Adrian Chapman
(
Oxford
)
08:00 - 10:00
Room: Zoom Room
Abstract: The Jordan-Wigner transformation represents a profound connection between the physics of many-body spin systems and the physics of fermionic systems. In the setting where the effective fermions are noninteracting, the Jordan-Wigner transformation gives an exact solution method for an otherwise apparently complicated spin model. I will describe a graph-theoretic framework which captures mappings to free fermions under a unified characterization, yielding new exact solutions to spin models. Remarkably, the relationships between exact-solution methods in this framework reflect the relationships between families of graphs. This suggests a promising approach to understanding the physics of many-body spin models through graph theory.
Thursday, 16 June 2022
Friday, 17 June 2022
08:00
A Graph-Theoretic Approach to Free-Fermion Solvability
-
Adrian Chapman
(
Oxford
)
A Graph-Theoretic Approach to Free-Fermion Solvability
Adrian Chapman
(
Oxford
)
08:00 - 10:00
Room: Zoom Room
Abstract: The Jordan-Wigner transformation represents a profound connection between the physics of many-body spin systems and the physics of fermionic systems. In the setting where the effective fermions are noninteracting, the Jordan-Wigner transformation gives an exact solution method for an otherwise apparently complicated spin model. I will describe a graph-theoretic framework which captures mappings to free fermions under a unified characterization, yielding new exact solutions to spin models. Remarkably, the relationships between exact-solution methods in this framework reflect the relationships between families of graphs. This suggests a promising approach to understanding the physics of many-body spin models through graph theory.
Saturday, 18 June 2022
Sunday, 19 June 2022
Monday, 20 June 2022
Tuesday, 21 June 2022
Wednesday, 22 June 2022
Thursday, 23 June 2022
Friday, 24 June 2022
Saturday, 25 June 2022
Sunday, 26 June 2022
Monday, 27 June 2022
Tuesday, 28 June 2022
14:00
The frontier of feebly interacting particles: from dark matter to the muon (g-2)
-
Luc Darmé
(
IP2I
)
The frontier of feebly interacting particles: from dark matter to the muon (g-2)
Luc Darmé
(
IP2I
)
14:00 - 16:00
Room: Zoom Room
New light but Feebly Interacting Particles (FIPs) represent an exciting and well-motivated class of new physics particles. FIPs are loosely defined as (1) singlets under the Standard Model (SM) gauge groups; (2) lighter than the electroweak scale and (3) not yet excluded or discovered. Many well-grounded new physics candidates fit this definition, with extremely bright experimental prospects for FIPs in the MeV and GeV mass range. In these lectures, we will present the theoretical foundations of this family of new physics particles and introduce some of its most searched-for members. The links between FIPs and the dark matter problem will be explored, along with their potential in explaining various low-energy experimental anomalies, including the measured anomalous magnetic moment.
Wednesday, 29 June 2022
Thursday, 30 June 2022
Friday, 1 July 2022
14:00
The frontier of feebly interacting particles: from dark matter to the muon (g-2)
-
Luc Darmé
(
IP2I
)
The frontier of feebly interacting particles: from dark matter to the muon (g-2)
Luc Darmé
(
IP2I
)
14:00 - 16:00
Room: Zoom Room
New light but Feebly Interacting Particles (FIPs) represent an exciting and well-motivated class of new physics particles. FIPs are loosely defined as (1) singlets under the Standard Model (SM) gauge groups; (2) lighter than the electroweak scale and (3) not yet excluded or discovered. Many well-grounded new physics candidates fit this definition, with extremely bright experimental prospects for FIPs in the MeV and GeV mass range. In these lectures, we will present the theoretical foundations of this family of new physics particles and introduce some of its most searched-for members. The links between FIPs and the dark matter problem will be explored, along with their potential in explaining various low-energy experimental anomalies, including the measured anomalous magnetic moment.
Saturday, 2 July 2022
Sunday, 3 July 2022
Monday, 4 July 2022
Tuesday, 5 July 2022
Wednesday, 6 July 2022
Thursday, 7 July 2022
Friday, 8 July 2022
Saturday, 9 July 2022
Sunday, 10 July 2022
Monday, 11 July 2022
Tuesday, 12 July 2022
Wednesday, 13 July 2022
Thursday, 14 July 2022
Friday, 15 July 2022
Saturday, 16 July 2022
Sunday, 17 July 2022
Monday, 18 July 2022
Tuesday, 19 July 2022
Wednesday, 20 July 2022
Thursday, 21 July 2022
Friday, 22 July 2022
Saturday, 23 July 2022
Sunday, 24 July 2022
Monday, 25 July 2022
Tuesday, 26 July 2022
Wednesday, 27 July 2022
Thursday, 28 July 2022
Friday, 29 July 2022
Saturday, 30 July 2022
Sunday, 31 July 2022
Monday, 1 August 2022
Tuesday, 2 August 2022
Wednesday, 3 August 2022
Thursday, 4 August 2022
Friday, 5 August 2022
Saturday, 6 August 2022
Sunday, 7 August 2022
Monday, 8 August 2022
Tuesday, 9 August 2022
Wednesday, 10 August 2022
Thursday, 11 August 2022
Friday, 12 August 2022
Saturday, 13 August 2022
Sunday, 14 August 2022
Monday, 15 August 2022
Tuesday, 16 August 2022
Wednesday, 17 August 2022
Thursday, 18 August 2022
Friday, 19 August 2022
Saturday, 20 August 2022
Sunday, 21 August 2022
Monday, 22 August 2022
Tuesday, 23 August 2022
Wednesday, 24 August 2022
Thursday, 25 August 2022
Friday, 26 August 2022
Saturday, 27 August 2022
Sunday, 28 August 2022
Monday, 29 August 2022
Tuesday, 30 August 2022
Wednesday, 31 August 2022
Thursday, 1 September 2022
Friday, 2 September 2022
Saturday, 3 September 2022
Sunday, 4 September 2022
Monday, 5 September 2022
Tuesday, 6 September 2022
Wednesday, 7 September 2022
Thursday, 8 September 2022
Friday, 9 September 2022
Saturday, 10 September 2022
Sunday, 11 September 2022
Monday, 12 September 2022
Tuesday, 13 September 2022
Wednesday, 14 September 2022
Thursday, 15 September 2022
Friday, 16 September 2022
Saturday, 17 September 2022
Sunday, 18 September 2022
Monday, 19 September 2022
Tuesday, 20 September 2022
Wednesday, 21 September 2022
Thursday, 22 September 2022
Friday, 23 September 2022
Saturday, 24 September 2022
Sunday, 25 September 2022
Monday, 26 September 2022
Tuesday, 27 September 2022
Wednesday, 28 September 2022
Thursday, 29 September 2022
Friday, 30 September 2022
Saturday, 1 October 2022
Sunday, 2 October 2022
Monday, 3 October 2022
Tuesday, 4 October 2022
Wednesday, 5 October 2022
Thursday, 6 October 2022
Friday, 7 October 2022
Saturday, 8 October 2022
Sunday, 9 October 2022
Monday, 10 October 2022
Tuesday, 11 October 2022
Wednesday, 12 October 2022
Thursday, 13 October 2022
Friday, 14 October 2022
Saturday, 15 October 2022
Sunday, 16 October 2022
Monday, 17 October 2022
Tuesday, 18 October 2022
Wednesday, 19 October 2022
Thursday, 20 October 2022
Friday, 21 October 2022
Saturday, 22 October 2022
Sunday, 23 October 2022
Monday, 24 October 2022
Tuesday, 25 October 2022
Wednesday, 26 October 2022
Thursday, 27 October 2022
Friday, 28 October 2022
Saturday, 29 October 2022
Sunday, 30 October 2022
Monday, 31 October 2022
Tuesday, 1 November 2022
Wednesday, 2 November 2022
Thursday, 3 November 2022
Friday, 4 November 2022
Saturday, 5 November 2022
Sunday, 6 November 2022
Monday, 7 November 2022
Tuesday, 8 November 2022
Wednesday, 9 November 2022
Thursday, 10 November 2022
Friday, 11 November 2022
Saturday, 12 November 2022
Sunday, 13 November 2022
Monday, 14 November 2022
Tuesday, 15 November 2022
Wednesday, 16 November 2022
Thursday, 17 November 2022
Friday, 18 November 2022
Saturday, 19 November 2022
Sunday, 20 November 2022
Monday, 21 November 2022
Tuesday, 22 November 2022
Wednesday, 23 November 2022
Thursday, 24 November 2022
Friday, 25 November 2022
Saturday, 26 November 2022
Sunday, 27 November 2022
Monday, 28 November 2022
Tuesday, 29 November 2022
Wednesday, 30 November 2022
Thursday, 1 December 2022
Friday, 2 December 2022
Saturday, 3 December 2022
Sunday, 4 December 2022
Monday, 5 December 2022
Tuesday, 6 December 2022
Wednesday, 7 December 2022
Thursday, 8 December 2022
Friday, 9 December 2022
Saturday, 10 December 2022
Sunday, 11 December 2022
Monday, 12 December 2022
Tuesday, 13 December 2022
Wednesday, 14 December 2022
Thursday, 15 December 2022
Friday, 16 December 2022
Saturday, 17 December 2022
Sunday, 18 December 2022
Monday, 19 December 2022
Tuesday, 20 December 2022
Wednesday, 21 December 2022
Thursday, 22 December 2022
Friday, 23 December 2022
Saturday, 24 December 2022
Sunday, 25 December 2022
Monday, 26 December 2022
Tuesday, 27 December 2022
Wednesday, 28 December 2022
Thursday, 29 December 2022
Friday, 30 December 2022
Saturday, 31 December 2022