In semiconductor physics, the flat band potential of a semiconductor defines the potential at which there is no depletion layer at the junction between a semiconductor and an electrolyte or p-n-junction. This is a consequence of the condition that the redox Fermi level of the electrolyte must be equal to the Fermi level of the semiconductor and therefore preventing any band bending of the conduction and valence band. An application of the flat band potential can be found in the determining the width of the space charge region in a semiconductor-electrolyte junction. Furthermore, it is used in the Mott-Schottky equation to determine the capacitance of the semiconductor-electrolyte junction and plays a role in the photocurrent of a photoelectrochemical cell. The value of the flat band potential depends on many factors, such as the material, pH and crystal structure of the material (Wikipedia).
Physics - E&M: Ch 38.1 Voltage Potential Understood (20 of 24) Determine Highest to Lowest Potential
Visit http://ilectureonline.com for more math and science lectures! In this video I will determine which corner of a square with 2 charges q and 2q is at the highest potential and then rank the rest of the corners from the highest to lowest potential. Next video in this series can be see
From playlist PHYSICS 38.1 VOLTAGE UNDERSTOOD
Bound State of the Delta Function Potential
We apply boundary conditions to find the bound state of the delta function potential.
From playlist Quantum Mechanics Uploads
Physics - E&M: Ch 38.1 Voltage Potential Understood (14 of 24) Potential inside a Conductor
Visit http://ilectureonline.com for more math and science lectures! In this video I will explain a graphical representation of what it means to have a potential inside a spherical conductor that carries a charge. Next video in this series can be seen at: https://youtu.be/dvja_zP2CI4
From playlist PHYSICS 38.1 VOLTAGE UNDERSTOOD
Physics - E&M: Ch 38.1 Voltage Potential Understood (13 of 24) Potential on Surface of a Conductor?
Visit http://ilectureonline.com for more math and science lectures! In this video I will explain the potential, V=?, at the surface of the sphere of a conductor that has additional charges on one side of the sphere. Next video in this series can be seen at: https://youtu.be/5EfuxYg03UM
From playlist PHYSICS 38.1 VOLTAGE UNDERSTOOD
Delta function potential I: Preliminaries
MIT 8.04 Quantum Physics I, Spring 2016 View the complete course: http://ocw.mit.edu/8-04S16 Instructor: Barton Zwiebach License: Creative Commons BY-NC-SA More information at http://ocw.mit.edu/terms More courses at http://ocw.mit.edu
From playlist MIT 8.04 Quantum Physics I, Spring 2016
Physics 38 Electrical Potential (12 of 22) Potential In-, On, & Outside a Spherical Conductor
Visit http://ilectureonline.com for more math and science lectures! In this video I will find the potential inside, at the surface, and outside of a spherical conductor.
From playlist PHYSICS 38 ELECTRICAL POTENTIAL
From playlist PHYS 102 | Current and Resistance
Flat bands in twisted bilayer transition metal dichalcogenides by Manish Jain
DISCUSSION MEETING NOVEL PHASES OF QUANTUM MATTER ORGANIZERS: Adhip Agarwala, Sumilan Banerjee, Subhro Bhattacharjee, Abhishodh Prakash and Smitha Vishveshwara DATE: 23 December 2019 to 02 January 2020 VENUE: Ramanujan Lecture Hall, ICTS Bangalore Recent theoretical and experimental
From playlist Novel Phases of Quantum Matter 2019
Stephen Carr: "A band-free approach to twistronics"
Theory and Computation for 2D Materials "A band-free approach to twistronics" Stephen Carr, Harvard University Abstract: Recent electronic models for moiré superlattices have provided accurate band structures to help guide experimental efforts. Unfortunately, calculating these band struc
From playlist Theory and Computation for 2D Materials 2020
Topology, correlations and superconductivity in magic angle..(Lecture 2) by Ashvin Vishwanath
INFOSYS-ICTS CHANDRASEKHAR LECTURES ENTANGLEMENT AND TOPOLOGY IN QUANTUM SOLIDS SPEAKER: Ashvin Vishwanath (Harvard University) DATE: 23 December 2019, 16:00 to 17:00 VENUE: Ramanujan lecture hall, ICTS campus Lecture 1 : Entanglement and Topology in Quantum Solids. Date & Time : Mon
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DISCUSSION MEETING NOVEL PHASES OF QUANTUM MATTER ORGANIZERS: Adhip Agarwala, Sumilan Banerjee, Subhro Bhattacharjee, Abhishodh Prakash and Smitha Vishveshwara DATE: 23 December 2019 to 02 January 2020 VENUE: Ramanujan Lecture Hall, ICTS Bangalore Recent theoretical and experimental
From playlist Novel Phases of Quantum Matter 2019
Topological and Flat Bands - Roderich Moessner
DISCUSSION MEETING : ADVANCES IN GRAPHENE, MAJORANA FERMIONS, QUANTUM COMPUTATION DATES Wednesday 19 Dec, 2012 - Friday 21 Dec, 2012 VENUE Auditorium, New Physical Sciences Building, IISc Quantum computation is one of the most fundamental and important research topics today, from both th
From playlist Advances in Graphene, Majorana fermions, Quantum computation
Flat bands in honeycomb networks by Masaki Oshikawa
DISCUSSION MEETING NOVEL PHASES OF QUANTUM MATTER ORGANIZERS: Adhip Agarwala, Sumilan Banerjee, Subhro Bhattacharjee, Abhishodh Prakash and Smitha Vishveshwara DATE: 23 December 2019 to 02 January 2020 VENUE: Ramanujan Lecture Hall, ICTS Bangalore Recent theoretical and experimental
From playlist Novel Phases of Quantum Matter 2019
Impurity effects on the superconductivity in twisted bilayer graphene by Fa Wang
DISCUSSION MEETING NOVEL PHASES OF QUANTUM MATTER ORGANIZERS: Adhip Agarwala, Sumilan Banerjee, Subhro Bhattacharjee, Abhishodh Prakash and Smitha Vishveshwara DATE: 23 December 2019 to 02 January 2020 VENUE: Ramanujan Lecture Hall, ICTS Bangalore Recent theoretical and experimental
From playlist Novel Phases of Quantum Matter 2019
2020 Theory Winter School: Oskar Vafek
Topic: Topology and interactions in twisted bilayer graphene narrow bands For more information on the 2020 Theory Winter School: https://nationalmaglab.org/news-events/events/for-scientists/winter-theory-school
From playlist 2020 Theory Winter School
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From playlist Physics
Physics 12.4.1b - Electric Potential and Potential Difference, continued
Continuation of the previous video. A discussion of electric potential and potential difference. High school difficulty level. From the physics course by Derek Owens. The distance learning course is available at http://www.derekowens.com
From playlist Physics - What is Voltage
Michael Weinstein - Discrete honeycombs, rational edges and edge states - IPAM at UCLA
Recorded 30 March 2022. Michael Weinstein of Columbia University, Applied Physics and Applied Mathematics, presents "Discrete honeycombs, rational edges and edge states" at IPAM's Multiscale Approaches in Quantum Mechanics Workshop. Abstract: We first discuss the derivation of tight bindin
From playlist 2022 Multiscale Approaches in Quantum Mechanics Workshop
Non-Hermitian Parity-Hole Symmetry, Flat Band, and Linear Localization by Li Ge
PROGRAM NON-HERMITIAN PHYSICS - PHHQP XVIII DATE :04 June 2018 to 13 June 2018 VENUE:Ramanujan Lecture Hall, ICTS Bangalore Non-Hermitian Physics-"Pseudo-Hermitian Hamiltonians in Quantum Physics (PHHQP) XVIII" is the 18th meeting in the series that is being held over the years in Qua
From playlist Non-Hermitian Physics - PHHQP XVIII
Thin Ring Electric Field using Electric Potential
First we solve for the electric potential along the axis of a uniform thin ring of electric charge. Then we use that electric potential to solve for the electric field at the same location. Want Lecture Notes? http://www.flippingphysics.com/thin-ring-electric-potential.html Chapters: 0:00
From playlist All of AP Physics C: Electricity & Magnetism!