Tatsu Takeuchi Virginia University, January 10, 2012.

Slides:



Advertisements
Similar presentations
Rae §2.1, B&J §3.1, B&M § An equation for the matter waves: the time-dependent Schrődinger equation*** Classical wave equation (in one dimension):
Advertisements

Introduction to Quantum Theory
Brane-World Inflation
Applying the Correspondence Principle to the Three-Dimensional Rigid Rotor David Keeports Mills College
The Wigner Function Chen Levi. Eugene Paul Wigner Received the Nobel Prize for Physics in
Chapter (6) Introduction to Quantum Mechanics.  is a single valued function, continuous, and finite every where.
Chapter 4 Free and Confined Electrons Lecture given by Qiliang Li Dept. of Electrical and Computer Engineering George Mason University ECE 685 Nanoelectronics.
1 Chapter 40 Quantum Mechanics April 6,8 Wave functions and Schrödinger equation 40.1 Wave functions and the one-dimensional Schrödinger equation Quantum.
Wavefunction Quantum mechanics acknowledges the wave-particle duality of matter by supposing that, rather than traveling along a definite path, a particle.
Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
String Theory Brian Bertrand.
Lecture 17: Intro. to Quantum Mechanics
Almost all detection of visible light is by the “photoelectric effect” (broadly defined.) There is always a threshold photon energy for detection, even.
Field Theory: The Past 25 Years Nathan Seiberg (IAS) The Future of Physics October, 2004 A celebration of 25 Years of.
Ch 9 pages ; Lecture 21 – Schrodinger’s equation.
Analysis of Microstructures and Phase Transition Phenomena contribution to Dynamic Days, Berlin, July 25-28, 2005 René J. Meziat, Jorge Villalobos Department.
Phase portraits of quantum systems Yu.A. Lashko, G.F. Filippov, V.S. Vasilevsky Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine.
CHAPTER 6 Quantum Mechanics II
Chang-Kui Duan, Institute of Modern Physics, CUPT 1 Harmonic oscillator and coherent states Reading materials: 1.Chapter 7 of Shankar’s PQM.
Holographic Description of Quantum Black Hole on a Computer Yoshifumi Hyakutake (Ibaraki Univ.) Collaboration with M. Hanada ( YITP, Kyoto ), G. Ishiki.
Particle in a Box - 1D (14.3) A simple problem that demonstrates the principles of quantum mechanics is the particle in a box (PIB) Inside the box of a.
Bound States 1. A quick review on the chapters 2 to Quiz Topics in Bound States:  The Schrödinger equation.  Stationary States.  Physical.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Background Independent Matrix Theory We parameterize the gauge fields by M transforms linearly under gauge transformations Gauge-invariant variables are.
Review : Quantum mechanics Jae-hoon Ji Nano Electro-Mechanical Device Lab.
Chapters Q6 and Q7 The Wavefunction and Bound Systems.
Chapter 41 1D Wavefunctions. Topics: Schrödinger’s Equation: The Law of Psi Solving the Schrödinger Equation A Particle in a Rigid Box: Energies and Wave.
Phy107 Fall Final Exam Thursday, Dec. 21: 2:45 - 4:45 pm 113 Psychology Building Note sheet: one double-sided page Cumulative exam-covers all material,
String Theory Mihir John What are the most basic constituents that make up the universe around us?
Matter Effect on Neutrino Oscillation from Universality Violation in Neutral Current Interactions Naotoshi Okamura (YITP) and Minako Honda (Ochanomizu.
Atomic Spectra and Atomic Energy States –
1 Honors Physics 1 Summary and Review - Fall 2013 Quantitative and experimental tools Mathematical tools Newton’s Laws and Applications –Linear motion.
Austin Hinkel Allyn Goatley Daniel Eigelbach
Chapter 5: Quantum Mechanics
Utrecht University Gerard ’t Hooft and Isaac Newton Institute, December 15, 2004.
Vibrational Motion Harmonic motion occurs when a particle experiences a restoring force that is proportional to its displacement. F=-kx Where k is the.
Quantum Two 1. 2 Time Independent Approximation Methods 3.
Quantum Chemistry: Our Agenda Postulates in quantum mechanics (Ch. 3) Schrödinger equation (Ch. 2) Simple examples of V(r) Particle in a box (Ch. 4-5)
Monday, Nov. 4, 2013PHYS , Fall 2013 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #15 Monday, Nov. 4, 2013 Dr. Jaehoon Yu Finite Potential.
Nanoelectronics Chapter 3 Quantum Mechanics of Electrons
CHAPTER 6 Quantum Mechanics II
Statistical physics in deformed spaces with minimal length Taras Fityo Department for Theoretical Physics, National University of Lviv.
Modern Physics lecture 4. The Schroedinger Equation As particles are described by a wave function, we need a wave equation for matter waves As particles.
5. The Harmonic Oscillator Consider a general problem in 1D Particles tend to be near their minimum Taylor expand V(x) near its minimum Recall V’(x 0 )
Holographic Description of Quantum Black Hole on a Computer Yoshifumi Hyakutake (Ibaraki Univ.) Collaboration with M. Hanada ( YITP, Kyoto ), G. Ishiki.
Cosmological Bell Inequalities Juan Maldacena AndyFest 2015 Warping the Universe: A celebration of the Science of Andrew Strominger.
Heavy quark energy loss in finite length SYM plasma Cyrille Marquet Columbia University based on F. Dominguez, C. Marquet, A. Mueller, B. Wu and B.-W.
Nanoelectronics Chapter 4 Free and Confined Electrons
Chapter 40 Quantum Mechanics
Schrödinger Representation – Schrödinger Equation
CHAPTER 5 The Schrodinger Eqn.
Joe Kapusta* University of Minnesota
Concept test 15.1 Suppose at time
A rotating hairy BH in AdS_3
Late-time Cosmology with String Gases
The Harmonic Oscillator
Peter Atkins • Julio de Paula Atkins’ Physical Chemistry
Concept test 15.1 Suppose at time
Quantum Two.
Peng Wang Sichuan University
CHAPTER 5 The Schrodinger Eqn.
Quantum mechanics II Winter 2012
Chapter 40 Quantum Mechanics
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103
Other examples of one-dimensional motion
EMERGENT CLASSICAL STRINGS
Stationary State Approximate Methods
Chapter 40 Quantum Mechanics
Linear Vector Space and Matrix Mechanics
Presentation transcript:

Tatsu Takeuchi Virginia University, January 10, 2012

Work in collaboration with: Zack Lewis Djordje Minic Lay Nam Chang Also contributions from: Naotoshi Okamura (Yamanashi Univ.) Sandor Benczik (quit physics) Saif Rayyan (MIT, physics education)

The Minimal Length Uncertainty Relation Suggested by Quantum Gravity. Observed in perturbative String Theory.

Deformed Commutation Relation

Harmonic Oscillator

Multi Dimensional Case

Isotropic Harmonic Oscillator in D dimensions

2D Case

Some Details (1D case) :

Solution:

Wave-functions: n=0 n=1 n=2

Uncertainties of the Harmonic Oscillator: β=0

Uncertainties of the Harmonic Oscillator: β≠0 How can we get onto the Δx~Δp branch?

Harmonic Oscillator with negative mass:

Uncertainties of the Harmonic Oscillator: β≠0, m<0

Classical Limit:

Classical Harmonic Oscillator:

m>0 case:

m  ∞  limit:

m<0 case:

Compactification:

Classical Probabilities:

Comparison with Quantum Probabilities:

Work in progress: Discreate energy eigenstates have been found for the negative mass case. Uncertainties are difficult to calculate. What do we mean by x=0 ?

The minimal length uncertainty relation allows discreate energy “bound” states for “inverted” potentials. In the classical limit, these “bound” states can be understood to be due to the finite time the particle spends near the phase-space origin. Particles move at arbitrary large velocites. Do the non- relativistic negative mass states correspond to relativistic imaginary mass tachyons? Conclusions: