In quantum mechanics, the Mott problem is a paradox that illustrates some of the difficulties of understanding the nature of wave function collapse and measurement in quantum mechanics. The problem was first formulated in 1929 by Sir Nevill Francis Mott and Werner Heisenberg, illustrating the paradox of the collapse of a spherically symmetric wave function into the linear tracks seen in a cloud chamber. In practice, virtually all high energy physics experiments, such as those conducted at particle colliders, involve wave functions which are inherently spherical. Yet, when the results of a particle collision are detected, they are invariably in the form of linear tracks (see, for example, the illustrations accompanying the article on bubble chambers). It is somewhat strange to think that a spherically symmetric wave function should be observed as a straight track, and yet, this occurs on a daily basis in all particle collider experiments. A related variant formulation was given in 1953 by Mauritius Renninger, and is now known as Renninger's negative-result gedanken experiment. In this formulation, it is noted that the absence of a particle detection can also constitute a quantum measurement; namely, that a measurement can be performed even if no particle whatsoever is detected. (Wikipedia).
An general explanation of the underactive thyroid.
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Continuous Mott transitions in a model Hamiltonian system by N S Vidhyadhiraja
29 May 2017 to 02 June 2017 VENUE: Ramanujan Lecture Hall, ICTS Bangalore This program aims to bring together people working on classical and quantum systems with disorder and interactions. The extensive exploration, through experiments, simulations and model calculations, of growing cor
From playlist Correlation and Disorder in Classical and Quantum Systems
Spontaneous disorder near the Mott transition on frustrated lattices by Pinaki Majumdar
29 May 2017 to 02 June 2017 VENUE: Ramanujan Lecture Hall, ICTS Bangalore This program aims to bring together people working on classical and quantum systems with disorder and interactions. The extensive exploration, through experiments, simulations and model calculations, of growing cor
From playlist Correlation and Disorder in Classical and Quantum Systems
Quantum critical Mott transitions in a bilayer Kondo insulator.....by N. S. Vidhyadhiraja
Indian Statistical Physics Community Meeting 2016 URL: https://www.icts.res.in/discussion_meeting/details/31/ DATES Friday 12 Feb, 2016 - Sunday 14 Feb, 2016 VENUE Ramanujan Lecture Hall, ICTS Bangalore This is an annual discussion meeting of the Indian statistical physics community wh
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Thank you to J.J. for sharing his story and if you're interested in more information about Child's Play, you can find them at http://childsplaycharity.org/ or https://twitter.com/CPCharity on Twitter. With the help of folks like you, they can continue to improve the lives of children in ho
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Dissipative Quantum Phase Transitions in Interacting Light-Matter Systems by Marco Schiro
Open Quantum Systems DATE: 17 July 2017 to 04 August 2017 VENUE: Ramanujan Lecture Hall, ICTS Bangalore There have been major recent breakthroughs, both experimental and theoretical, in the field of Open Quantum Systems. The aim of this program is to bring together leaders in the Open Q
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From playlist MOOC on Emergency Surgical Conditions
A non-Hermitian Hamiltonian description of the dynamic Mott transition by Vikram Tripathi
DATES Monday 20 Jun, 2016 - Wednesday 29 Jun, 2016 VENUE Ramanujan Lecture Hall, ICTS Bangalore APPLY Understanding strongly interacting quantum many body systems is one of the major frontiers in present day physics. Condensed matter physics provides a wide panoply of systems where strong
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Example problem solving a system of linear differential equations.
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Learn about the movement for women's equality that precipitated the Seneca Falls Convention in 1848, and what its attendees - including Elizabeth Cady Stanton and Lucretia Mott - hoped to achieve. Subscribe for more HISTORY: http://histv.co/SubscribeHistoryYT Newsletter: https://www.hist
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PROGRAM: The ICTS Condensed Matter Programme 2011 Venue: Indian Insitute of Science, Bangalore Date: Friday 09 Dec, 2011 - Thursday 22 Dec, 2011 DESCRIPTION: The ICTS Condensed Matter Programme 2011 (ICMP 2011) consists of a 10 day Winter School (December 9 to December 18) followed by a 4
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Quantum Spin Liquids in Kagome Lattice by Subhro Bhattacharjee
29 May 2017 to 02 June 2017 VENUE: Ramanujan Lecture Hall, ICTS Bangalore This program aims to bring together people working on classical and quantum systems with disorder and interactions. The extensive exploration, through experiments, simulations and model calculations, of growing cor
From playlist Correlation and Disorder in Classical and Quantum Systems
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The diagnosis of acute appendicitis remains clinical. There are a variety of special investigations, though, to confirm the diagnosis, aid in determining the extent of the disease and in diagnosing alternate conditions.
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C49 Example problem solving a system of linear DEs Part 1
Solving an example problem of a system of linear differential equations, where one of the equations is not homogeneous. It's a long problem, so this is only part 1.
From playlist Differential Equations
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Solving a differential equation by separating the variables.
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MIT 8.422 Atomic and Optical Physics II, Spring 2013 View the complete course: http://ocw.mit.edu/8-422S13 Instructor: Wolfgang Ketterle In this lecture, the professor discussed ideal Bose gases, weakly interacting homogenous Bose gas, inhomogenous Bose gas, etc. License: Creative Common
From playlist MIT 8.422 Atomic and Optical Physics II, Spring 2013