UGC ACADEMY LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM PH 05 PHYSICAL SCIENCE TEST SERIES # 1. Quantum, Statistical & Thermal Physics
|
|
- Helena Ellis
- 5 years ago
- Views:
Transcription
1 UGC ACADEMY LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM BOOKLET CODE SUBJECT CODE PH 05 PHYSICAL SCIENCE TEST SERIES # Quantum, Statistical & Thermal Physics Timing: 3: H M.M: 00 Instructions. This test paper has a total of 50 questions. All Questions are compulsory.. Each questions are 4 marks 3. Read the Questions carefully and mark your appropriate response to the OMR sheet. 4. There is Negative marking of /4 for each wrong answer. 5. Mark the response by Black or Blue Ball Pen only. 6. Calculator and mobile phone is not allowed during exam
2 . The state of a quantum mechanical system is described by a wave function. Consider two physical observables that have discrete eigenvalues: observable A with eigenvalues {α}, and observable B with eigenvalues {β}. Under what circumstances can all wave functions be expanded in a set of basis states, each of which is a simultaneous eigenfunction of both A and B? (a) Only if the values {α} and {β} are nondegenerate (b) Only if A and B commute (c) Only if A commutes with the Hamitonian of the system (d) Only if B commutes with the Hamiltonian of the system. An ensemble of quantum harmonic oscillator is kept at a finite temperature T / kb Energy level of a Single oscillator is n, specific heat varies with temperature (T) at kt is (a) T (b) (c) (d) independent of T 3. Variational parameter of a particle of mass m in the potential V ( x) x 6m normalized trial wave function /4 / ( x) e x, is,value of n is (a) (b) / (c) /3 (d) 4, estimated using the 4. A measurement of energy E will always satisfy which of the following relationships? (a) E π²ħ²/8ma² (b) E π²ħ²/ma² (c) E = π²ħ²/8ma² (d) E = π²ħ²/ma² 5. A very simple square well potential is given x 0 V ( x) 0 0 x L x L Density of state of this quantum system depend on (a) L (b) (c) (d) 6. A system containing two identical particles is described by a wave function of the form ( x ) ( x) ( x ) ( x) Where x and x represent the spatial coordinates of the particles and α and β represent all the quantum numbers, including spin, of the states that they occupy. The particles might be (a) Electrons (b) Positrons (c) Protons (d) Deuterons
3 7. The figure above shows one of the possible energy eigenfunctions ψ(x) for a particle bouncing freely back and forth along the x-axis between impenetrable walls located at x = a and x = +a. The potential energy equals zero for x > a. If the energy of the particle is electron volts when it is in the quantum state associated with this eigenfunction, what is its energy when it is in the quantum state of lowest possible energy? (a) 0 ev (b) / ev (c). / ev (d) ev 8. The state in equation is linear combination of three orthonormal eigenstates 6 3 of the operator corresponding to eigenvalues -, and. What is the expectation value of for this state? (a) /3 (b) (7/6) (c) (d) 4/3 9. Which of the following functions could represent the radial wave function for an electron in an atom? (r is the distance of the electron from the nucleus; A and b are constants.) I. Ae br II. A sin (br) III. A/r (a) I only (b) II only (c) I and II only (d) I and III only 0. A particle of mass m is in a potential V m x, where is a constant. Let. = In the Heisenberg picture is given by (a) (b) i (c) - (d) - i. In one dimension, two metal A and B have Fermi temperature of free electron in ratio :4 ratio of number of electron per unit area is (a) :3 (b) : (c) :8 (d) :4. Hamiltonian of matrix 0 H 0 0 0
4 energy eigen value correct to I st order in perturbation is (a) 0,, (b) 0, (c) 0, 3, (d) 0, 3. If the Pressure of a free electron gas in - Dimension is increased by 8 times, its electron density change by (a) (b) 4 (c) 8 (d) 6 4. We have a planer sheet of Silicin gas (single layer of silicon, which treated as -D system).fill electron following dispersion relation, c is a constant, electron density of electron varies with T n, T is temp. of system, n is (a) 0 (b) (c) (d) ½ 5. Pressure of a non-relativistic free Fermi gas in one dimension depends at T 0, varies with particle density as (a) 53 n (b) (c) /3 n (d) 6. A system can have three energy levels: E = 0,. The level E=0 is doubly degenerate, while the others are non-degenerate. The specific heat at inverse temperature is (b). (d) None 7. A particle of mass m in three dimensions is in the potential n Ratio of ground states energy to first excited state energy is (a) (b) (c) (d) 8. Given that r the uncertainty p r in the ground state o(r) = of the hydrogen atom by uncertainty principle is( ) (b). (c) (d). 9. Consider black body radiation contained in a cavity whose walls are at temperature T. The radiation is in equilibrium with the walls of the cavity. If the temperature of the walls is increased to T and the radiation is allowed to come to equilibrium at the new temperature, the number of photon of the radiation increases by a factor of (a) (b) 4 (c) 8 (d) 6
5 0. The Coulomb potential V(r) = - of a hydrogen atom is perturbed by adding (where c is a constant) to the Hamiltonian. The first order correction to the ground state energy is in state (a) c (b) 4c (c) - 4c (d) none. The electron in newly discovered two-dimensional gas MoS with a linear energy-momentum relation. A is constant, If is the number of electrons per unit area, Energy density is proportional to (a) 3/ (b) (c) /3 (d). The Hamiltonian for a spin-/ particle at rest is given by, where and are Pauli spin matrices and A isconstants. The eigenvalues of this Hamiltonian are (a) (b) (c) A(doubly degenerate) (d) 3. At time t 0a particle in the potential ( x,0) A ( ) n ( x) n n V x m x ( ) / is described by the wave function Where n( x ) are eigenstates of the energy with eigenvalues En n. You are given that ( n, n' ) nn'. What is normalization constant A (a) (b) (c) m (d) none of these 4. Consider a linear harmonic oscillator and Let, 0 and be its real, normalized ground and first excited state energy eigenfunctions respectively. Let A0 B with A and B real numbers be the wave function of the oscillator at some instant of time. is maximum if (a) AB (b) AB (c) A B (d) A B 5. Consider electron in graphene obey dispersion relation of electron is proportional to wave vector (k) over the entire k-space, ground state energy per electron of system in term of Fermi energy is (a) E F (b) E F (c) E F (d) E F 6. The wave function for a particle confined to a one-dimensional box located between x = 0 and x = L is Ψ(x) =A sin (n π x/l) + B cos (n π x/l). The constants A and B are determined to be
6 (a),0 (b), (c) 0, (d), 7. Let represent the state of an electron with spin up and the state of an electron with spin down. Valid spin eigenfunctions for a triplet state I. II. 3 ( S ) of a two-electron atom include which of the following? (a) I only (b) II only (c) III only (d) I and III III. 8. A particle of mass m is acted on by a harmonic force with potential energy function V(x) = mω²x²/ (a one dimensional simple harmonic oscillator). If there is a wall at x = 0 so that V = for x < 0, then the energy levels are equals to (a) 0, ħω, ħω,... (b) 0, ¹ ₂ħω, ħω,... (c) ¹ ₂ħω, ³ ₂ħω, ⁵ ₂ħω,... (d) ³ ₂ħω, ⁷ ₂ħω, ¹¹ ₂ħω, The raising and lowering operators for the quantum harmonic oscillator satisfy a n ( n ) n a n n n for energy eigenstates n with energy E n. Which of the following gives the first-order shift in the n energy level due to the perturbation H V( a a ) where V is constant? (a) 0 (b) V (c) V (d) 5V 30. The operator a (defind bellow) when operating on a harmonic energy eigenstate ψ n with energy E n, produces another energy eigenstate whose energy is E n ħω 0. Which of the following is true? m 0 p a x i m 0 I. a commutes with the Hamiltonian. II. a is a Hermitian operator and therefore an observable. III. The adjoint operator a a (a) I only (b) II only (c) III only (d) I and II only
7 3. A Classical model of a diatomic molecule is a springy dumbbell, as shown above, where the dumbbell is free to rotate about axes perpendicular to the spring. In the limit of high temperature, what is the specific heat per mole at constant volume? (a) 3/ R (b) 5/ (c) 7/ R (d) 9/ R 3. A sample of N atoms of helium gas is confined in a.0 cubic meter volume. The probability that none of the helium atoms is in a 0 6 cubic meter volume of the container is (a) zero (b) 0 6 (c) ( 0 6 ) N (d) (0 6 ) N 33. For a system in which the number of particles is fixed, the reciprocal of the Kelvin temperature T is given by which of the following derivatives? (Let P= pressure, V = volume, S = entropy, and U = internal energy.) (a) ( P/ V) S (b) ( P/ S) V (c) ( V/ P) U (d) ( S/ U) V 34. A large isolated of N weakly interacting particles is in thermal equilibrium. Each particle has only 3 possible non degenerate states of energies 0, ε, and 3ε. When the system is at an absolute temperature T ε/k, where k is Boltzmann s constant, the average energy of each particle is (a) zero (b) ε (c) 4ε /3 (d) 3ε 35. In a gas of N diatomic molecules, two possible models for a classical description of a diatomic molecule are: Which of the following statements about this gas is true? (a) Model I has a specific heat c v = ³ ₂Nk (b) Model II has a smaller specific heat than Model I (c) Model II is always correct (d) The choice between Models I and II depends on the temperature 36. If the absolute temperature of a blackbody is increased by a factor of 3, the energy radiated per second per unit area does which of the following (a) Decreases by a factor of 8 (b) Decreases by a factor of 9 (c) Increases by a factor of 9 (d) Increases by a factor of The solution to the Schrödinger equation for a particle bound in a one-dimensional, infinitely deep potential well, indexed by quantum number n, indicates that in the middle of the well the probability density vanishes for (a) The ground state (n = ) only (b) States of even n (n =, 4,...) (c) States of odd n (n =, 3,...) (d) All states (n =,, 3,...)
8 38. At a given instant of time, a rigid rotator is in the state ψ(θ, ϕ) = (¾π) sin θ sin ϕ, where θ is the polar angle relative to the z-axis and ϕ is the azimuthal angle. Measurement will find which of the following possible values of the z-component of the angular momentum L z? (a) 0 (b) ħ/, ħ/ (c) ħ, ħ (d) ħ, ħ 39. For an ideal diatomic gas in thermal equilibrium, the ratio of the molar heat capacity at constant volume at very high temperatures to that at very low temperatures is equal to (a) 3 (b) 5/3 (c) (d) 7/3 40. A diatomic molecules is initially in the state Ψ(Θ, Φ) = (5Y + 3Y 5 + Y 5 ) / (38) ½ where Y l m is a spherical harmonics. If measurements are made of the total angular momentum quantum number l and of azimuthal angular momentum quantum number m, what is the probability of obtaining the results l = 5? (a) 36/444 (b) 9/38 (c)3/38 (d) 5/(38) ½ 4. Suppose an e is in a state describe by the wave function Where g( r) r dr and polar, and azimuthal angles. 0 What is probability when m 0 (a) (b) 3 ( i e sin cos ) g ( r ) 4 (c) 3 4. A particle of mass is confined to a one dimensional region as (d) none At its normalized wave function is 8 x x ( x,0) cos sin 5a a a What is probability corresponding to (a) 0.8 (b) 0.6 (c) 0.64 (d) A quantum-mechanical state of a particle with cartesian coordinate x,y,z is described by the normalised / wave fucntion ( x, y, z) Az exp ( x y z ) Expectation value of L is (a) 0 (b) (c) (d) 6
9 3 44. We have a multiwall carbon nanotube, which follows the dispersion relation ( k) k over the enitre k- space fermi energy ( F ) depends on e density of electron (a) /3 /3 3 (b) (c) (d) 45. Suppose ( x,0) x A a For a and A are constant. What is x (a) a (b) a (c) a (d) a 46. Suppose you are given the following relation among the entropy S, volume V, internal energy E, number of particle N of a thermodynamics system 3 S A( NVU ) Relation between pressure (p) to temperature (T) is (a) p T (b) p /3 T (c) p 3/ T (d) p T 47. For a quantum mechanical harmonic oscillators with energy En n n 0,,,... Chemical potential of system is (a) sinh (c) KT n sinh (b) (d) NKT n sinh NK cot n sinh 48. If a particle is represented by unnormalised wave function C ( ) 5 a x x a ( x) a 0 x a Ground state energy of system is (a) (b) (c) (d)
10 49. An is confined to the interior of a hollow spherical cavity of radius with impenetrable walls expression for pressure exerted on walls of cavity by in its ground state is varies with radius as (a) (b) (c) (d) In case of spherical,pressure is independent of radius 50. The wave function ψ(x) = A exp ( b x /), where A and b are real constants, is a normalized eigenfunction of the Schrodinger equation for a particle of mass M and energy E in a one dimensional potential V(x) such that V(x) = 0 at x = 0. Which of the following is correct? (a) V = ħ b 4 /M (b) V = ħ b 4 x /M (c) V = ħ b 6 x 4 /M (d) E = ħ b ( b x ) Good luck ANSWERKEY. (b). (d) 3. (c) 4. (b) 5. (a) 6. (d) 7. (c) 8. (c) 9. (a) 0. (b). (d). (b) 3. (a) 4. (d) 5. (b) 6. (c) 7. (b) 8. (d) 9. (c) 0. (b). (a). (a) 3. (b) 4. (c) 5. (c) 6. () 7. (d) 8. (d) 9. (d) 30. (c) 3. (c) 3. (c) 33. (d) 34. (c) 35. (d) 36. (d) 37. (b) 38. (c) 39. (d) 40. (c) 4. (c) 4. (d) 43. (b) 44. (b) 45. (a) 46. (c) 47. (c) 48. (a) 49. (c) 50. (b)
SCIENCE VISION INSTITUTE For CSIR NET/JRF, GATE, JEST, TIFR & IIT-JAM Web:
Test Series: CSIR NET/JRF Exam Physical Sciences Test Paper: Quantum Mechanics-I Instructions: 1. Attempt all Questions. Max Marks: 185 2. There is a negative marking of 1/4 for each wrong answer. 3. Each
More informationUGC ACADEMY LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM PHYSICAL SCIENCE TEST SERIES # 4. Atomic, Solid State & Nuclear + Particle
UGC ACADEMY LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM BOOKLET CODE PH PHYSICAL SCIENCE TEST SERIES # 4 Atomic, Solid State & Nuclear + Particle SUBJECT CODE 05 Timing: 3: H M.M: 200 Instructions 1.
More informationThe general solution of Schrödinger equation in three dimensions (if V does not depend on time) are solutions of time-independent Schrödinger equation
Lecture 17 Page 1 Lecture 17 L17.P1 Review Schrödinger equation The general solution of Schrödinger equation in three dimensions (if V does not depend on time) is where functions are solutions of time-independent
More informationProblems and Multiple Choice Questions
Problems and Multiple Choice Questions 1. A momentum operator in one dimension is 2. A position operator in 3 dimensions is 3. A kinetic energy operator in 1 dimension is 4. If two operator commute, a)
More informationProblem 1: Spin 1 2. particles (10 points)
Problem 1: Spin 1 particles 1 points 1 Consider a system made up of spin 1/ particles. If one measures the spin of the particles, one can only measure spin up or spin down. The general spin state of a
More informationQualifying Exam. Aug Part II. Please use blank paper for your work do not write on problems sheets!
Qualifying Exam Aug. 2015 Part II Please use blank paper for your work do not write on problems sheets! Solve only one problem from each of the four sections Mechanics, Quantum Mechanics, Statistical Physics
More informationPhysics PhD Qualifying Examination Part I Wednesday, January 21, 2015
Physics PhD Qualifying Examination Part I Wednesday, January 21, 2015 Name: (please print) Identification Number: STUDENT: Designate the problem numbers that you are handing in for grading in the appropriate
More informationPHYS3113, 3d year Statistical Mechanics Tutorial problems. Tutorial 1, Microcanonical, Canonical and Grand Canonical Distributions
1 PHYS3113, 3d year Statistical Mechanics Tutorial problems Tutorial 1, Microcanonical, Canonical and Grand Canonical Distributions Problem 1 The macrostate probability in an ensemble of N spins 1/2 is
More informationQuantum Physics 130A. April 1, 2006
Quantum Physics 130A April 1, 2006 2 1 HOMEWORK 1: Due Friday, Apr. 14 1. A polished silver plate is hit by beams of photons of known energy. It is measured that the maximum electron energy is 3.1 ± 0.11
More informationLecture #1. Review. Postulates of quantum mechanics (1-3) Postulate 1
L1.P1 Lecture #1 Review Postulates of quantum mechanics (1-3) Postulate 1 The state of a system at any instant of time may be represented by a wave function which is continuous and differentiable. Specifically,
More informationJoint Entrance Examination for Postgraduate Courses in Physics EUF
Joint Entrance Examination for Postgraduate Courses in Physics EUF Second Semester 013 Part 1 3 April 013 Instructions: DO NOT WRITE YOUR NAME ON THE TEST. It should be identified only by your candidate
More informationTime part of the equation can be separated by substituting independent equation
Lecture 9 Schrödinger Equation in 3D and Angular Momentum Operator In this section we will construct 3D Schrödinger equation and we give some simple examples. In this course we will consider problems where
More informationChemistry 3502/4502. Final Exam Part I. May 14, 2005
Chemistry 3502/4502 Final Exam Part I May 14, 2005 1. For which of the below systems is = where H is the Hamiltonian operator and T is the kinetic-energy operator? (a) The free particle (e) The
More informationChemistry 3502/4502. Final Exam Part I. May 14, 2005
Advocacy chit Chemistry 350/450 Final Exam Part I May 4, 005. For which of the below systems is = where H is the Hamiltonian operator and T is the kinetic-energy operator? (a) The free particle
More informationInternational Physics Course Entrance Examination Questions
International Physics Course Entrance Examination Questions (May 2010) Please answer the four questions from Problem 1 to Problem 4. You can use as many answer sheets you need. Your name, question numbers
More informationψ s a ˆn a s b ˆn b ψ Hint: Because the state is spherically symmetric the answer can depend only on the angle between the two directions.
1. Quantum Mechanics (Fall 2004) Two spin-half particles are in a state with total spin zero. Let ˆn a and ˆn b be unit vectors in two arbitrary directions. Calculate the expectation value of the product
More informationIntroduction to Quantum Mechanics PVK - Solutions. Nicolas Lanzetti
Introduction to Quantum Mechanics PVK - Solutions Nicolas Lanzetti lnicolas@student.ethz.ch 1 Contents 1 The Wave Function and the Schrödinger Equation 3 1.1 Quick Checks......................................
More informationChem 452 Mega Practice Exam 1
Last Name: First Name: PSU ID #: Chem 45 Mega Practice Exam 1 Cover Sheet Closed Book, Notes, and NO Calculator The exam will consist of approximately 5 similar questions worth 4 points each. This mega-exam
More informationUniversity of Michigan Physics Department Graduate Qualifying Examination
Name: University of Michigan Physics Department Graduate Qualifying Examination Part II: Modern Physics Saturday 17 May 2014 9:30 am 2:30 pm Exam Number: This is a closed book exam, but a number of useful
More informationQuantum Physics III (8.06) Spring 2007 FINAL EXAMINATION Monday May 21, 9:00 am You have 3 hours.
Quantum Physics III (8.06) Spring 2007 FINAL EXAMINATION Monday May 21, 9:00 am You have 3 hours. There are 10 problems, totalling 180 points. Do all problems. Answer all problems in the white books provided.
More informationThe general solution of Schrödinger equation in three dimensions (if V does not depend on time) are solutions of time-independent Schrödinger equation
Lecture 27st Page 1 Lecture 27 L27.P1 Review Schrödinger equation The general solution of Schrödinger equation in three dimensions (if V does not depend on time) is where functions are solutions of time-independent
More informationMathematical Tripos Part IB Michaelmas Term Example Sheet 1. Values of some physical constants are given on the supplementary sheet
Mathematical Tripos Part IB Michaelmas Term 2015 Quantum Mechanics Dr. J.M. Evans Example Sheet 1 Values of some physical constants are given on the supplementary sheet 1. Whenasampleofpotassiumisilluminatedwithlightofwavelength3
More informationPHYSICAL SCIENCES MODEL QUESTION PAPER PART A PART B
PHYSICAL SCIENCES This Test Booklet will contain 65 ( Part `A + Part `B+5 Part C ) Multiple Choice Questions (MCQs). Candidates will be required to answer 5 in part A, in Part B and questions in Part C
More informationOne-electron Atom. (in spherical coordinates), where Y lm. are spherical harmonics, we arrive at the following Schrödinger equation:
One-electron Atom The atomic orbitals of hydrogen-like atoms are solutions to the Schrödinger equation in a spherically symmetric potential. In this case, the potential term is the potential given by Coulomb's
More informationPhysics 228 Today: Ch 41: 1-3: 3D quantum mechanics, hydrogen atom
Physics 228 Today: Ch 41: 1-3: 3D quantum mechanics, hydrogen atom Website: Sakai 01:750:228 or www.physics.rutgers.edu/ugrad/228 Happy April Fools Day Example / Worked Problems What is the ratio of the
More informationClassical Mechanics Comprehensive Exam
Name: Student ID: Classical Mechanics Comprehensive Exam Spring 2018 You may use any intermediate results in the textbook. No electronic devices (calculator, computer, cell phone etc) are allowed. For
More informationProblem 1: A 3-D Spherical Well(10 Points)
Problem : A 3-D Spherical Well( Points) For this problem, consider a particle of mass m in a three-dimensional spherical potential well, V (r), given as, V = r a/2 V = W r > a/2. with W >. All of the following
More informationC. Show your answer in part B agrees with your answer in part A in the limit that the constant c 0.
Problem #1 A. A projectile of mass m is shot vertically in the gravitational field. Its initial velocity is v o. Assuming there is no air resistance, how high does m go? B. Now assume the projectile is
More information1. Estimate the lifetime of an excited state of hydrogen. Give your answer in terms of fundamental constants.
Sample final questions.. Estimate the lifetime of an excited state of hydrogen. Give your answer in terms of fundamental constants. 2. A one-dimensional harmonic oscillator, originally in the ground state,
More information(a) Write down the total Hamiltonian of this system, including the spin degree of freedom of the electron, but neglecting spin-orbit interactions.
1. Quantum Mechanics (Spring 2007) Consider a hydrogen atom in a weak uniform magnetic field B = Bê z. (a) Write down the total Hamiltonian of this system, including the spin degree of freedom of the electron,
More informationLecture 5: Harmonic oscillator, Morse Oscillator, 1D Rigid Rotor
Lecture 5: Harmonic oscillator, Morse Oscillator, 1D Rigid Rotor It turns out that the boundary condition of the wavefunction going to zero at infinity is sufficient to quantize the value of energy that
More informationThermal and Statistical Physics Department Exam Last updated November 4, L π
Thermal and Statistical Physics Department Exam Last updated November 4, 013 1. a. Define the chemical potential µ. Show that two systems are in diffusive equilibrium if µ 1 =µ. You may start with F =
More informationJ10M.1 - Rod on a Rail (M93M.2)
Part I - Mechanics J10M.1 - Rod on a Rail (M93M.2) J10M.1 - Rod on a Rail (M93M.2) s α l θ g z x A uniform rod of length l and mass m moves in the x-z plane. One end of the rod is suspended from a straight
More informationMath Questions for the 2011 PhD Qualifier Exam 1. Evaluate the following definite integral 3" 4 where! ( x) is the Dirac! - function. # " 4 [ ( )] dx x 2! cos x 2. Consider the differential equation dx
More information= ( Prove the nonexistence of electron in the nucleus on the basis of uncertainty principle.
Worked out examples (Quantum mechanics). A microscope, using photons, is employed to locate an electron in an atom within a distance of. Å. What is the uncertainty in the momentum of the electron located
More informationPotential energy, from Coulomb's law. Potential is spherically symmetric. Therefore, solutions must have form
Lecture 6 Page 1 Atoms L6.P1 Review of hydrogen atom Heavy proton (put at the origin), charge e and much lighter electron, charge -e. Potential energy, from Coulomb's law Potential is spherically symmetric.
More informationPHY413 Quantum Mechanics B Duration: 2 hours 30 minutes
BSc/MSci Examination by Course Unit Thursday nd May 4 : - :3 PHY43 Quantum Mechanics B Duration: hours 3 minutes YOU ARE NOT PERMITTED TO READ THE CONTENTS OF THIS QUESTION PAPER UNTIL INSTRUCTED TO DO
More informationIntroduction to Quantum Mechanics (Prelude to Nuclear Shell Model) Heisenberg Uncertainty Principle In the microscopic world,
Introduction to Quantum Mechanics (Prelude to Nuclear Shell Model) Heisenberg Uncertainty Principle In the microscopic world, x p h π If you try to specify/measure the exact position of a particle you
More informationPHY 407 QUANTUM MECHANICS Fall 05 Problem set 1 Due Sep
Problem set 1 Due Sep 15 2005 1. Let V be the set of all complex valued functions of a real variable θ, that are periodic with period 2π. That is u(θ + 2π) = u(θ), for all u V. (1) (i) Show that this V
More informationQuantum Mechanics Solutions
Quantum Mechanics Solutions (a (i f A and B are Hermitian, since (AB = B A = BA, operator AB is Hermitian if and only if A and B commute So, we know that [A,B] = 0, which means that the Hilbert space H
More informationCHAPTER 6 Quantum Mechanics II
CHAPTER 6 Quantum Mechanics II 6.1 The Schrödinger Wave Equation 6.2 Expectation Values 6.3 Infinite Square-Well Potential 6.4 Finite Square-Well Potential 6.5 Three-Dimensional Infinite-Potential Well
More informationJoint Entrance Examination for Postgraduate Courses in Physics EUF
Joint Entrance Examination for Postgraduate Courses in Physics EUF First Semester/01 Part 1 4 Oct 011 Instructions: DO NOT WRITE YOUR NAME ON THE TEST. It should be identified only by your candidate number
More informationM04M.1 Particles on a Line
Part I Mechanics M04M.1 Particles on a Line M04M.1 Particles on a Line Two elastic spherical particles with masses m and M (m M) are constrained to move along a straight line with an elastically reflecting
More informationProblem #1 30 points Problem #2 30 points Problem #3 30 points Problem #4 30 points Problem #5 30 points
Name ME 5 Exam # November 5, 7 Prof. Lucht ME 55. POINT DISTRIBUTION Problem # 3 points Problem # 3 points Problem #3 3 points Problem #4 3 points Problem #5 3 points. EXAM INSTRUCTIONS You must do four
More informationChem 467 Supplement to Lecture 19 Hydrogen Atom, Atomic Orbitals
Chem 467 Supplement to Lecture 19 Hydrogen Atom, Atomic Orbitals Pre-Quantum Atomic Structure The existence of atoms and molecules had long been theorized, but never rigorously proven until the late 19
More informationCollection of formulae Quantum mechanics. Basic Formulas Division of Material Science Hans Weber. Operators
Basic Formulas 17-1-1 Division of Material Science Hans Weer The de Broglie wave length λ = h p The Schrödinger equation Hψr,t = i h t ψr,t Stationary states Hψr,t = Eψr,t Collection of formulae Quantum
More informationMATH325 - QUANTUM MECHANICS - SOLUTION SHEET 11
MATH35 - QUANTUM MECHANICS - SOLUTION SHEET. The Hamiltonian for a particle of mass m moving in three dimensions under the influence of a three-dimensional harmonic oscillator potential is Ĥ = h m + mω
More informationPh.D. Comprehensive Exam Department of Physics Georgetown University
Ph.D. Comprehensive Exam Department of Physics Georgetown University Part I: Tuesday, July 10, 2018, 12:00pm - 4:00pm Proctors: Mak Paranjape and Ed Van Keuren Instructions: Please put your assigned number
More informationColumbia University Department of Physics QUALIFYING EXAMINATION
Columbia University Department of Physics QUALIFYING EXAMINATION Wednesday, January 12, 2011 1:00PM to 3:00PM Modern Physics Section 3. Quantum Mechanics Two hours are permitted for the completion of this
More informationPhysics Qual - Statistical Mechanics ( Fall 2016) I. Describe what is meant by: (a) A quasi-static process (b) The second law of thermodynamics (c) A throttling process and the function that is conserved
More informationQuantum Theory of Angular Momentum and Atomic Structure
Quantum Theory of Angular Momentum and Atomic Structure VBS/MRC Angular Momentum 0 Motivation...the questions Whence the periodic table? Concepts in Materials Science I VBS/MRC Angular Momentum 1 Motivation...the
More informationSpin Dynamics Basic Theory Operators. Richard Green SBD Research Group Department of Chemistry
Spin Dynamics Basic Theory Operators Richard Green SBD Research Group Department of Chemistry Objective of this session Introduce you to operators used in quantum mechanics Achieve this by looking at:
More information1 Commutators (10 pts)
Final Exam Solutions 37A Fall 0 I. Siddiqi / E. Dodds Commutators 0 pts) ) Consider the operator  = Ĵx Ĵ y + ĴyĴx where J i represents the total angular momentum in the ith direction. a) Express both
More informationQuantum Mechanics Solutions. λ i λ j v j v j v i v i.
Quantum Mechanics Solutions 1. (a) If H has an orthonormal basis consisting of the eigenvectors { v i } of A with eigenvalues λ i C, then A can be written in terms of its spectral decomposition as A =
More informationPreliminary Examination - Day 2 August 16, 2013
UNL - Department of Physics and Astronomy Preliminary Examination - Day August 16, 13 This test covers the topics of Quantum Mechanics (Topic 1) and Thermodynamics and Statistical Mechanics (Topic ). Each
More informationPhysics 107 Final Exam May 6, Your Name: 1. Questions
Physics 107 Final Exam May 6, 1996 Your Name: 1. Questions 1. 9. 17. 5.. 10. 18. 6. 3. 11. 19. 7. 4. 1. 0. 8. 5. 13. 1. 9. 6. 14.. 30. 7. 15. 3. 8. 16. 4.. Problems 1. 4. 7. 10. 13.. 5. 8. 11. 14. 3. 6.
More informationThe 3 dimensional Schrödinger Equation
Chapter 6 The 3 dimensional Schrödinger Equation 6.1 Angular Momentum To study how angular momentum is represented in quantum mechanics we start by reviewing the classical vector of orbital angular momentum
More information2016 Lloyd G. Elliott University Prize Exam Compiled by the Department of Physics & Astronomy, University of Waterloo
Canadian Association of Physicists SUPPORTING PHYSICS RESEARCH AND EDUCATION IN CANADA 2016 Lloyd G. Elliott University Prize Exam Compiled by the Department of Physics & Astronomy, University of Waterloo
More informationk m Figure 1: Long problem L2 2 + L2 3 I 1
LONG PROBLEMS 1: Consider the system shown in Figure 1: Two objects, of mass m 1 and m, can be treated as point-like. Each of them is suspended from the ceiling by a wire of negligible mass, and of length
More informationStatistical Mechanics
Statistical Mechanics Newton's laws in principle tell us how anything works But in a system with many particles, the actual computations can become complicated. We will therefore be happy to get some 'average'
More informationBasic Quantum Mechanics
Frederick Lanni 10feb'12 Basic Quantum Mechanics Part I. Where Schrodinger's equation comes from. A. Planck's quantum hypothesis, formulated in 1900, was that exchange of energy between an electromagnetic
More informationThermal & Statistical Physics Study Questions for the Spring 2018 Department Exam December 6, 2017
Thermal & Statistical Physics Study Questions for the Spring 018 Department Exam December 6, 017 1. a. Define the chemical potential. Show that two systems are in diffusive equilibrium if 1. You may start
More informationQualifying Exam for Ph.D. Candidacy Department of Physics October 11, 2014 Part I
Qualifying Exam for Ph.D. Candidacy Department of Physics October 11, 214 Part I Instructions: The following problems are intended to probe your understanding of basic physical principles. When answering
More informationChapter 4 (Lecture 6-7) Schrodinger equation for some simple systems Table: List of various one dimensional potentials System Physical correspondence
V, E, Chapter (Lecture 6-7) Schrodinger equation for some simple systems Table: List of various one dimensional potentials System Physical correspondence Potential Total Energies and Probability density
More information1. Electricity and Magnetism (Fall 1995, Part 1) A metal sphere has a radius R and a charge Q.
1. Electricity and Magnetism (Fall 1995, Part 1) A metal sphere has a radius R and a charge Q. (a) Compute the electric part of the Maxwell stress tensor T ij (r) = 1 {E i E j 12 } 4π E2 δ ij both inside
More informationUNIVERSITY OF SURREY FACULTY OF ENGINEERING AND PHYSICAL SCIENCES DEPARTMENT OF PHYSICS. BSc and MPhys Undergraduate Programmes in Physics LEVEL HE2
Phys/Level /1/9/Semester, 009-10 (1 handout) UNIVERSITY OF SURREY FACULTY OF ENGINEERING AND PHYSICAL SCIENCES DEPARTMENT OF PHYSICS BSc and MPhys Undergraduate Programmes in Physics LEVEL HE PAPER 1 MATHEMATICAL,
More informationUNIVERSITY OF MISSOURI-COLUMBIA PHYSICS DEPARTMENT. PART I Qualifying Examination. January 20, 2015, 5:00 p.m. to 8:00 p.m.
UNIVERSITY OF MISSOURI-COLUMBIA PHYSICS DEPARTMENT PART I Qualifying Examination January 20, 2015, 5:00 p.m. to 8:00 p.m. Instructions: The only material you are allowed in the examination room is a writing
More informationPHYS 771, Quantum Mechanics, Final Exam, Fall 2011 Instructor: Dr. A. G. Petukhov. Solutions
PHYS 771, Quantum Mechanics, Final Exam, Fall 11 Instructor: Dr. A. G. Petukhov Solutions 1. Apply WKB approximation to a particle moving in a potential 1 V x) = mω x x > otherwise Find eigenfunctions,
More informationCHAPTER 8 The Quantum Theory of Motion
I. Translational motion. CHAPTER 8 The Quantum Theory of Motion A. Single particle in free space, 1-D. 1. Schrodinger eqn H ψ = Eψ! 2 2m d 2 dx 2 ψ = Eψ ; no boundary conditions 2. General solution: ψ
More informationChemistry 120A 2nd Midterm. 1. (36 pts) For this question, recall the energy levels of the Hydrogenic Hamiltonian (1-electron):
April 6th, 24 Chemistry 2A 2nd Midterm. (36 pts) For this question, recall the energy levels of the Hydrogenic Hamiltonian (-electron): E n = m e Z 2 e 4 /2 2 n 2 = E Z 2 /n 2, n =, 2, 3,... where Ze is
More informationPhysics PhD Qualifying Examination Part I Wednesday, August 26, 2015
Physics PhD Qualifying Examination Part I Wednesday, August 26, 2015 Name: (please print) Identification Number: STUDENT: Designate the problem numbers that you are handing in for grading in the appropriate
More information8 Wavefunctions - Schrödinger s Equation
8 Wavefunctions - Schrödinger s Equation So far we have considered only free particles - i.e. particles whose energy consists entirely of its kinetic energy. In general, however, a particle moves under
More informationQUANTUM MECHANICS SECOND EDITION G. ARULDHAS
QUANTUM MECHANICS SECOND EDITION G. ARULDHAS Formerly, Professor and Head of Physics and Dean, Faculty of Science University of Kerala New Delhi-110001 2009 QUANTUM MECHANICS, 2nd Ed. G. Aruldhas 2009
More informationChemistry 532 Practice Final Exam Fall 2012 Solutions
Chemistry 53 Practice Final Exam Fall Solutions x e ax dx π a 3/ ; π sin 3 xdx 4 3 π cos nx dx π; sin θ cos θ + K x n e ax dx n! a n+ ; r r r r ˆL h r ˆL z h i φ ˆL x i hsin φ + cot θ cos φ θ φ ) ˆLy i
More informationEXAM INFORMATION. Radial Distribution Function: B is the normalization constant. d dx. p 2 Operator: Heisenberg Uncertainty Principle:
EXAM INFORMATION Radial Distribution Function: P() r RDF() r Br R() r B is the normalization constant., p Operator: p ^ d dx Heisenberg Uncertainty Principle: n ax n! Integrals: xe dx n1 a x p Particle
More information8.04: Quantum Mechanics Professor Allan Adams Massachusetts Institute of Technology Wednesday April Exam 2
8.04: Quantum Mechanics Professor Allan Adams Massachusetts Institute of Technology Wednesday April 18 2012 Exam 2 Last Name: First Name: Check Recitation Instructor Time R01 Barton Zwiebach 10:00 R02
More informationGS-2017-Y (Physics) TATA INSTITUTE OF FUNDAMENTAL RESEARCH. Wrtten Test in PHYSICS December 11, 2016 Duration : 3 (Three) Hours
GS-2017-Y (Physics) TATA INSTITUTE OF FUNDAMENTAL RESEARCH Wrtten Test in PHYSICS December 11, 2016 Duration : 3 (Three) Hours NAME: REF. CODE: Please Read These Instructions Carefully Before Attempting
More informationQUANTUM MECHANICS. Franz Schwabl. Translated by Ronald Kates. ff Springer
Franz Schwabl QUANTUM MECHANICS Translated by Ronald Kates Second Revised Edition With 122Figures, 16Tables, Numerous Worked Examples, and 126 Problems ff Springer Contents 1. Historical and Experimental
More informationThe Schrödinger Equation
Chapter 13 The Schrödinger Equation 13.1 Where we are so far We have focused primarily on electron spin so far because it s a simple quantum system (there are only two basis states!), and yet it still
More informationChemistry 483 Lecture Topics Fall 2009
Chemistry 483 Lecture Topics Fall 2009 Text PHYSICAL CHEMISTRY A Molecular Approach McQuarrie and Simon A. Background (M&S,Chapter 1) Blackbody Radiation Photoelectric effect DeBroglie Wavelength Atomic
More informationPhysics 828 Problem Set 7 Due Wednesday 02/24/2010
Physics 88 Problem Set 7 Due Wednesday /4/ 7)a)Consider the proton to be a uniformly charged sphere of radius f m Determine the correction to the s ground state energy 4 points) This is a standard problem
More informationatoms and light. Chapter Goal: To understand the structure and properties of atoms.
Quantum mechanics provides us with an understanding of atomic structure and atomic properties. Lasers are one of the most important applications of the quantummechanical properties of atoms and light.
More information( r) = 1 Z. e Zr/a 0. + n +1δ n', n+1 ). dt ' e i ( ε n ε i )t'/! a n ( t) = n ψ t = 1 i! e iε n t/! n' x n = Physics 624, Quantum II -- Exam 1
Physics 624, Quantum II -- Exam 1 Please show all your work on the separate sheets provided (and be sure to include your name) You are graded on your work on those pages, with partial credit where it is
More informationPRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in
LONDON BEIJING HONG TSINGHUA Report and Review in Physics Vol2 PRINCIPLES OF PHYSICS From Quantum Field Theory to Classical Mechanics Ni Jun Tsinghua University, China NEW JERSEY \Hp SINGAPORE World Scientific
More informationPH 451/551 Quantum Mechanics Capstone Winter 201x
These are the questions from the W7 exam presented as practice problems. The equation sheet is PH 45/55 Quantum Mechanics Capstone Winter x TOTAL POINTS: xx Weniger 6, time There are xx questions, for
More informationParticle in one-dimensional box
Particle in the box Particle in one-dimensional box V(x) -a 0 a +~ An example of a situation in which only bound states exist in a quantum system. We consider the stationary states of a particle confined
More informationA few principles of classical and quantum mechanics
A few principles of classical and quantum mechanics The classical approach: In classical mechanics, we usually (but not exclusively) solve Newton s nd law of motion relating the acceleration a of the system
More informationApplications of Quantum Theory to Some Simple Systems
Applications of Quantum Theory to Some Simple Systems Arbitrariness in the value of total energy. We will use classical mechanics, and for simplicity of the discussion, consider a particle of mass m moving
More informationChemistry 881 Lecture Topics Fall 2001
Chemistry 881 Lecture Topics Fall 2001 Texts PHYSICAL CHEMISTRY A Molecular Approach McQuarrie and Simon MATHEMATICS for PHYSICAL CHEMISTRY, Mortimer i. Mathematics Review (M, Chapters 1,2,3 & 4; M&S,
More informationPHYSICS 721/821 - Spring Semester ODU. Graduate Quantum Mechanics II Midterm Exam - Solution
PHYSICS 72/82 - Spring Semester 2 - ODU Graduate Quantum Mechanics II Midterm Exam - Solution Problem ) An electron (mass 5, ev/c 2 ) is in a one-dimensional potential well as sketched to the right (the
More informationAnswer TWO of the three questions. Please indicate on the first page which questions you have answered.
STATISTICAL MECHANICS June 17, 2010 Answer TWO of the three questions. Please indicate on the first page which questions you have answered. Some information: Boltzmann s constant, kb = 1.38 X 10-23 J/K
More informationApplied Nuclear Physics (Fall 2006) Lecture 8 (10/4/06) Neutron-Proton Scattering
22.101 Applied Nuclear Physics (Fall 2006) Lecture 8 (10/4/06) Neutron-Proton Scattering References: M. A. Preston, Physics of the Nucleus (Addison-Wesley, Reading, 1962). E. Segre, Nuclei and Particles
More informationGraduate Written Examination Fall 2014 Part I
Graduate Written Examination Fall 2014 Part I University of Minnesota School of Physics and Astronomy Aug. 19, 2014 Examination Instructions Part 1 of this exam consists of 10 problems of equal weight.
More informationDEPARTMENT OF PHYSICS BROWN UNIVERSITY Written Qualifying Examination for the Ph.D. Degree January 23, 2009 READ THESE INSTRUCTIONS CAREFULLY
DEPARTMENT OF PHYSICS BROWN UNIVERSITY Written Qualifying Examination for the Ph.D. Degree January 23, 2009 READ THESE INSTRUCTIONS CAREFULLY 1. The time allowed to complete the exam is 12:00 5:00 PM.
More informationPhys 622 Problems Chapter 5
1 Phys 622 Problems Chapter 5 Problem 1 The correct basis set of perturbation theory Consider the relativistic correction to the electron-nucleus interaction H LS = α L S, also known as the spin-orbit
More informationECE440 Nanoelectronics. Lecture 07 Atomic Orbitals
ECE44 Nanoelectronics Lecture 7 Atomic Orbitals Atoms and atomic orbitals It is instructive to compare the simple model of a spherically symmetrical potential for r R V ( r) for r R and the simplest hydrogen
More informationComplementi di Fisica Lectures 10-11
Complementi di Fisica - Lectures 1-11 15/16-1-1 Complementi di Fisica Lectures 1-11 Livio Lanceri Università di Trieste Trieste, 15/16-1-1 Course Outline - Reminder Quantum Mechanics: an introduction Reminder
More informationLecture 4 Quantum mechanics in more than one-dimension
Lecture 4 Quantum mechanics in more than one-dimension Background Previously, we have addressed quantum mechanics of 1d systems and explored bound and unbound (scattering) states. Although general concepts
More information3.024 Electrical, Optical, and Magnetic Properties of Materials Spring 2012 Recitation 8 Notes
Overview 1. Electronic Band Diagram Review 2. Spin Review 3. Density of States 4. Fermi-Dirac Distribution 1. Electronic Band Diagram Review Considering 1D crystals with periodic potentials of the form:
More informationSolutions to exam : 1FA352 Quantum Mechanics 10 hp 1
Solutions to exam 6--6: FA35 Quantum Mechanics hp Problem (4 p): (a) Define the concept of unitary operator and show that the operator e ipa/ is unitary (p is the momentum operator in one dimension) (b)
More information