Quantum basics Definition and 86 Threads
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 29: Representing a moving particle by a wave packet
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 30: Stationary-state Schrodinger equation
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 31: Solution of the stationary-state Schrodinger equation for a SHO
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 32: Equivalance of Heisenberg and the Schrodinger formulations I
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 33: Equivalance of Heisenberg and Schrodinger formulations II
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 34: Born interpretation of the wavefunction
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 35: Uncertainty principle and its simple applications
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 36: Time dependent Schrodinger equation
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 37: Ehrenfest theorem
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 38: Solution of Schrodinger equation for a particle in delta functions
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 39: Solution of Schrodinger equation for a particle in a finite well
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 40: Solution of a one dimensional Schrodinger equation for bound states I
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 41: Solution of a one dimensional Schrodinger equation for bound states II
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 42: Reflection and transmission of particles across a potential barrier
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 43: Quantum-tunneling and its examples
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 44: Solution of the Schrodinger for free paticles and periodic boundary cond
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 45: Electrons in a metal : Density of states and Fermi energy
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 46: Schrodinger equation for particles in spherically symmetric potential
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 47: Angular momentum operator and its eigenfunctions
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 48: Equation for radial component of the wavefunction
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 49: Solution for radial component of the wavefunction for the hydrogen atom
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 50: Soln. for radial component of wavefunction for spherically sym potential
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 51: Bloch's theorem
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 52: Kroning-Penny model and energy bands
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 53: Kroning-Penny model with periodic Dirac delta function and energy bands
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 54: Discussion on Bands
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 55: Summary of the Course
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 4: Black Body Radiation IV
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Introductory Quantum Mechanics with Prof. Manoj Harbola (NPTEL):- Lecture 5: Black Body Radiation V
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I How Do Indices Determine Positions in a Quantum Density Matrix?
I am reading Leonard Susskind's Theoretical Minimum book on Quantum Mechanics. Excercise 7.4 is as follows: Calculate the density matrix for ##|\Psi\rangle = \alpha|u\rangle + \beta|d\rangle##. Answer: $$ \psi(u) = \alpha, \quad \psi^*(u) = \alpha^* \\ \psi(d) = \beta, \quad \psi^*(d) =...- doggydan42
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- Density Density matrix Indices Matrix Quantum basics
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I Double-Slit Interference w/ Separate Sources
If you have two similar coherent sources which are separated from each other by a barrier. Now one source sends particles one by one into one slit and the other sends particles into the other in a double slit interference experiment. Now, the photons are always undistinguishable, so they should...- Adiater
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- Coherent Double slit interference Interference Photons Quantum basics Sources
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- Forum: Quantum Physics
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Question on correctly interpreting a bra-ket equation
I am trying to solve for the uncertainty in energy ##\Delta E## in the following exercise: $$\Delta E = \sqrt{\langle \Phi | (\hat H - \bar E )^2 | \Phi \rangle}$$ Questions What does ##(\hat H - \bar E )^2## mean? Is it a simple binomial expansion into ##\hat H^2 - 2 \bar E \hat H + \bar...- blaisem
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- Bra-ket Quantum basics
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- Forum: Introductory Physics Homework Help
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I For a particle on a sphere, is zero energy possible?
In my introduction to quantum mechanics, I learned about the particle in a box, followed by the quantum harmonic oscillator. In both instances, zero energy was not possible; the ground states had non-zero energy. However, in deriving the solutions to the Schrödinger equation for a particle on a...- blaisem
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- Energy Particle Quantum basics Sphere Zero
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What's the energy-spread of the quantum Universe state?
If the universe was in an energy eigenstate then d<A>/dt = 0 for any dynamic variable A. Stuff moves which implies that the Universe isn't in an eigenstate. What factors drive the energy spread?- Robert Shaw
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- Cosmology Quantum Quantum basics State Universe
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I Trouble understanding the idea of a cavity radiator being a Black Body
I have been trying to understand the role of a cavity as a black body radiator in the derivation of planks black body radiation law but it has left me with 5 main questions: 1. If an object is a perfect absorber it must also be a perfect emitter, meaning that (allowing for a cavity not being a...- kal
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- Black body Black body radiation Body Cavity Emissivity Idea Quantum basics Radiator Thermodaynamics Thermodyamics
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I Physical interpretation of a Hamiltonian with a constraint
Dear physics forums, What is the physical interpretation of imposing the following constrain on a Hamiltonian: Tr(\hat H^2)=2\omega ^2 where \omega is a given constant. I am not very familiar with why is the trace of the hamiltonian there. Thanks in advance, Alex- Alex Cros
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- Constraint Hamiltonian Interpretation Physical Quantum basics Quantum theory
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- Forum: Quantum Interpretations and Foundations