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Today's Topics:
1. Автобус 03.10 (Наталья Медведева)
2. Friday 03.10.2025 (Stanislav Apostolov)
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Message: 1
Date: Thu, 2 Oct 2025 17:06:33 +0300
From: Наталья Медведева <nmedvedeva@itp.ac.ru>
To: seminars@itp.ac.ru, staff@itp.ac.ru, students@itp.ac.ru
Subject: [Landau ITP Seminars] Автобус 03.10
Message-ID: <6a52e440-888b-45d4-adff-5bbb386540de@itp.ac.ru>
Content-Type: text/plain; charset=UTF-8; format=flowed
Уважаемые сотрудники и студенты!
На завтра 03.10.25г. в 10-05 автобус запланирован.
Место сбора 11-я парковая, поворот на Щелковское шоссе.
Форд-Транзит А 797МА 150
тел. 8-903-019-86-80
Владимир Николаевич
С уважением
Н. Н.
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Message: 2
Date: Thu, 02 Oct 2025 19:25:02 +0300
From: Stanislav Apostolov <sapostolov@itp.ac.ru>
To: Students <students@itp.ac.ru>, Staff <staff@itp.ac.ru>, Seminars
<seminars@itp.ac.ru>
Subject: [Landau ITP Seminars] Friday 03.10.2025
Message-ID: <46165763d3ab56e3f46cb5a8ba1ea349@itp.ac.ru>
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Уважаемые коллеги!
На заседании Ученого совета ИТФ в пятницу 03.10 будет заслушан доклад:
11:30
M. A. Skvortsov, A. V. Polkin
Thermal phase slips in superconducting films and Boussinesq equation
A dissipationless supercurrent state in superconductors can be destroyed
by thermal fluctuations. Thermally activated phase slips provide a
finite resistance of the sample and are responsible for dark counts in
superconducting single photon detectors. The activation barrier for a
phase slip is determined by a space-dependent saddle-point (instanton)
configuration of the order parameter. In the one-dimensional wire
geometry, such a saddle point has been analytically obtained by Langer
and Ambegaokar in the vicinity of the critical temperature, $T_c$, and
for arbitrary bias currents below the critical current $I_c$. In the
two-dimensional geometry of a superconducting strip, which is relevant
for photon detection, the situation is much more complicated. Depending
on the ratio $I/I_c$, several types of saddle-point configurations have
been proposed, with their energies being obtained numerically. We
demonstrate that the saddle-point configuration for an infinite
superconducting film at $I\to I_c$ is described by the exactly
integrable Boussinesq equation solved by Hirota's method. The
instanton size is $L_x\sim\xi(1-I/I_c)^{-1/4}$ along the current and
$L_y\sim\xi(1-I/I_c)^{-1/2}$ perpendicular to the current, where $\xi$
is the Ginzburg-Landau coherence length. The activation energy for
thermal phase slips scales as $\Delta F^\text{2D}\propto
(1-I/I_c)^{3/4}$. For sufficiently wide strips of width $w\gg L_y$, a
half-instanton is formed near the boundary, with the activation energy
being 1/2 of $\Delta F^\text{2D}$.
ID и пароль онлайн-трансляций в Zoom те же, что и для предыдущих
трансляций семинаров и докладов на Ученом совете:
https://zoom.us/j/96899364518?pwd=MzBsR2lYT0lYL2x2b1oyNU9LeWlWUT09
Meeting ID: 968 9936 4518
Пароль: 250319
Просьба присутствовать на заседании членов Учёного совета в связи с
голосование открытым, поднятием "виртуальной" руки.
На завтра 03.10.25г. в 10-05 автобус запланирован.
Место сбора 11-я парковая, поворот на Щелковское шоссе.
Форд-Транзит А 797МА 150
тел. 8-903-019-86-80
Владимир Николаевич
Links:
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[1]
https://yandex.ru/maps/213/moscow/?from=mapframe&indoorLevel=1&ll=37.804151%2C55.809870&mode=usermaps&source=mapframe&um=constructor%3A1gjtTU9HvRzE3mvpCCP6B_Io424BFoMD&utm_source=mapframe&z=17.4
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