MATH2999 Directed Studies in Mathematics Quantum Process on One Qubit System Name: Au Tung Kin UID: 2009264740.

Slides:



Advertisements
Similar presentations
Example: Given a matrix defining a linear mapping Find a basis for the null space and a basis for the range Pamela Leutwyler.
Advertisements

Quantum Computing MAS 725 Hartmut Klauck NTU
Introduction to Quantum Information Processing CS 467 / CS 667 Phys 467 / Phys 767 C&O 481 / C&O 681 Lecture 11 (2005) Richard Cleve DC 3524
Linear Transformations
DENSITY MATRICES, traces, Operators and Measurements
Advanced Computer Architecture Lab University of Michigan Quantum Operations and Quantum Noise Dan Ernst Quantum Noise and Quantum Operations Dan Ernst.
Quantum Error Correction Michele Mosca. Quantum Error Correction: Bit Flip Errors l Suppose the environment will effect error (i.e. operation ) on our.
Chapter 6 Eigenvalues.
Quantum Computing Lecture 22 Michele Mosca. Correcting Phase Errors l Suppose the environment effects error on our quantum computer, where This is a description.
Introduction to Quantum Information Processing Lecture 4 Michele Mosca.
Dirac Notation and Spectral decomposition Michele Mosca.
Quantum Mechanics from Classical Statistics. what is an atom ? quantum mechanics : isolated object quantum mechanics : isolated object quantum field theory.
Dirac Notation and Spectral decomposition
Introduction to Quantum logic (2) Yong-woo Choi.
quantum computing |Y0 U H H-1 Y|A|Y quantum-bit (qubit) 0  
Presented by: Erik Cox, Shannon Hintzman, Mike Miller, Jacquie Otto, Adam Serdar, Lacie Zimmerman.
1 Introduction to Quantum Information Processing CS 667 / PH 767 / CO 681 / AM 871 Richard Cleve DC 2117 Lecture 14 (2009)
Linear Algebra Review 1 CS479/679 Pattern Recognition Dr. George Bebis.
IPQI-2010-Anu Venugopalan 1 Quantum Mechanics for Quantum Information & Computation Anu Venugopalan Guru Gobind Singh Indraprastha Univeristy Delhi _______________________________________________.
Alice and Bob’s Excellent Adventure
Generalized Deutsch Algorithms IPQI 5 Jan Background Basic aim : Efficient determination of properties of functions. Efficiency: No complete evaluation.
ME 1202: Linear Algebra & Ordinary Differential Equations (ODEs)
1 Introduction to Quantum Information Processing CS 667 / PH 767 / CO 681 / AM 871 Richard Cleve DC 2117 Lecture 20 (2009)
8.4.2 Quantum process tomography 8.5 Limitations of the quantum operations formalism 量子輪講 2003 年 10 月 16 日 担当:徳本 晋
IPQI-2010-Anu Venugopalan 1 qubits, quantum registers and gates Anu Venugopalan Guru Gobind Singh Indraprastha Univeristy Delhi _______________________________________________.
An Introduction to Quantum Computation Sandy Irani Department of Computer Science University of California, Irvine.
Richard Cleve DC 2117 Introduction to Quantum Information Processing QIC 710 / CS 667 / PH 767 / CO 681 / AM 871 Lecture (2011)
Density matrix and its application. Density matrix An alternative of state-vector (ket) representation for a certain set of state-vectors appearing with.
COMPUTER FUNDAMENTALS David Samuel bhatti
Beyond Vectors Hung-yi Lee. Introduction Many things can be considered as “vectors”. E.g. a function can be regarded as a vector We can apply the concept.
Quantum Shift Register Circuits Mark M. Wilde arXiv: National Institute of Standards and Technology, Wednesday, June 10, 2009 To appear in Physical.
Singular Value Decomposition and its applications
Eigenfaces (for Face Recognition)
Inverse of a Matrix Hung-yi Lee Textbook: Chapter 2.3, 2.4 Outline:
CS479/679 Pattern Recognition Dr. George Bebis
Postulates of Quantum Mechanics
Linear Algebra Linear Transformations. 2 Real Valued Functions Formula Example Description Function from R to R Function from to R Function from to R.
The Matrix of a Linear Transformation (9/30/05)
LINEAR TRANSFORMATIONS
§3-3 realization for multivariable systems
Systems of First Order Linear Equations
Quantum One.
Quantum One.
Quantum One.
Linear Transformations
For computer scientists
Complex Analysis in Quantum Computing
Quantum One.
Lecture on Linear Algebra
A Ridiculously Brief Overview
Numerical Ranges in Modern Times 14th WONRA at Man-Duen Choi
CS485/685 Computer Vision Dr. George Bebis
Quantum One.
Introduction to Quantum logic (2)
Quantum One.
Singular Value Decomposition SVD
OSU Quantum Information Seminar
Determinants CHANGE OF BASIS © 2016 Pearson Education, Inc.
Maths for Signals and Systems Linear Algebra in Engineering Lectures 13 – 14, Tuesday 8th November 2016 DR TANIA STATHAKI READER (ASSOCIATE PROFFESOR)
Linear Transformations
Linear Vector Space and Matrix Mechanics
University of Queensland
Subject :- Applied Mathematics
Linear Vector Space and Matrix Mechanics
NULL SPACES, COLUMN SPACES, AND LINEAR TRANSFORMATIONS
Vector Spaces COORDINATE SYSTEMS © 2012 Pearson Education, Inc.
Linear Equations in Linear Algebra
Linear Equations in Linear Algebra
Quantum One.
Presentation transcript:

MATH2999 Directed Studies in Mathematics Quantum Process on One Qubit System Name: Au Tung Kin UID: 2009264740

Abstracts Background Quantum system of Mixed Quantum States Program of Constructing TPCP Map Special Techniques in Program Acknowledgements Reference

Background: History & New Hope 1st Generation Vacuum Tubes 3rd Generation Integrated Circuits (IC) 2nd Generation Transistor Quantum Computer!!! Computer in the future? 5th Generation Artificial Intelligence (AI) 4th Generation Microprocessor

Background: Quantum Computer VS Classical Computer Comparisons between UNIT for storing information Qubit Bit Represent “1” or “0” Represent “1” or “0” ONLY e.g. Circuit Signals e.g. Spin of electrons Superposition of “1” and “0” 1 1 1

Background: Quantum Computer Qubit: the unit of storing information Three superconducting qubits. Credits: IBM research Quantum Operations Unitary Transformation Unitary Linear Mapping :C2  C2 vector space e.g. A unitary transformation Pauli-x Operation i.e. x transforms “1” to “0” i.e. x transforms “0” to “1” x : Quantum NOT Gate

Quantum system of Mixed Quantum States Experiment Interesting Situations Environment time = 0 time = t Time We know the state !!!Experimenter performs operations on the original state!!! We (included the experimenter) do NOT know the operations Answer: The new state can be describe by density matrix

Quantum system of Mixed Quantum States Interesting Situations time = 0 time = t Time We know the probability of the state at time t: e.g. The New State (MIXED) at time t: (2x2 Density Matrix)

Quantum system of Mixed Quantum States Given 2x2 density matrices A1 , A2 , A3 , A4  H2x2 B1 , B2 , B3 , B4  H2x2 Does a linear TPCP map T: H2x2  H2x2 s.t. T(Ai)=Bi always exists? Quantum system of Mixed Quantum States Can we describe the operations in mathematics? Interesting Situations Experiment time = 0 Environment time = t Time The operations on density matrices: Trace-Preserving -Completely-Positive linear map (TPCP map) A linearly completely positive map is trace-preserving:

Program of Constructing TPCP Map A program was developed Given density matrices as domain elements and images Construct a linear TPCP map if it exists Show notice if TPCP map does not exists

How to Construct TPCP Map? Given n density matrices, A1, A2, … , An  H2x2 TPCP Map T: H2x2  H2x2    B1, B2, … , Bn  H2x2 are their corresponding images Procedure 1: Find out all linearly independent Ai’s Procedure 2: Check linear coefficients preserve among Ai’s and Bi’s Procedure 3: Construct TPCP map for linearly independent Ai’s and corresponding Bi’s

How to Construct TPCP Map? Procedure 2: Linear Coefficient Preserve 2nd Step Check linear coefficient preserve or not e.g. Suppose where and A4 is dependent of and i.e. A3 = 1 + 2 Necessary Condition!  B3 = 1 + 2 Hence, if A3 = 1 + 2 But B3 ≠ 1 + 2 Then linear map for T(Ai) = Bi must not exist!

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Let k be the number of linearly independent Ai’s Since are Ai H2x2 where H2x2 is a vector space with dimensions 4 k can be at most 4 Divide k into 4 cases k = 1 k = 2 k = 3 k = 4

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 1: k = 1 Given A1 , B1  H2x2 Find a TPCP map T : H2x2  H2x2 s.t. T(A1) = B1 TPCP map T : H2x2  H2x2 T(X) = trace(X) B1

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 2: k = 2 Given A1 , A2 , B1 , B2  H2x2 Find a TPCP map T : H2x2  H2x2 s.t. T(Ai) = Bi for i = 1, 2 A1 = where x1 is 2x1 column vector with norm 1 A2 = where x2 is 2x1 column vector with norm 1 B1 = B2 =

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 2: k = 2

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 2: k = 2 Put X = A1 = x1 x1* + B1

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 2: k = 2 Put X = A2 = x2 x2* +

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 3: k = 3 Given A1 , A2 , A3 , B1 , B2 , B3  H2x2 Find a TPCP map T : H2x2  H2x2 s.t. T(Ai) = Bi for i = 1, 2, 3 A1 = where x1 is 2x1 column vector with norm 1 A2 = where x2 is 2x1 column vector with norm 1 A3 = where x3 is 2x1 column vector with norm 1 x3

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 3: k = 3 If there exists a 2x2 matrix C s.t. 1. trace(CC*) = 1+|det(C)|2  2 2. 3.

How to Construct TPCP Map How to Construct TPCP Map? Procedure 3: TPCP Map for Linearly Independent Case 4: k = 4 Given Ai , Bi  H2x2 for i = 1, 2, 3, 4 Find a TPCP map T : H2x2  H2x2 s.t. T(Ai) = Bi for i = 1, 2, 3, 4 There is one unique linear map T : H2x2  H2x2 If the unique linear map satisfy 1. Trace-Preserving 2. Completely-Positive It is the required TPCP map! is positive semi-definite or not

Acknowledgements Thank all for coming this seminar! Thank all for your kind attention! Besides,…… Thank Prof. Li, Prof. Poon, Dr Chan and Dr Cheung for their support!!!

Reference Timeline of computer chronicle IBM makes significant breakthrough towards scalable quantum computers http://www.zmescience.com/research/ibm- quantum-computer-28022012/ The atomic structure of individual nanoparticles http://nycgrp.wordpress.com/2011/05/18/

Reference Environment http://informedfarmers.com/nrm/environment/ File:Military laser experiment.jpg http://en.wikipedia.org/wiki/File:Military_laser_e xperiment.jpg

THE END!