Complexity Zoology
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Computational Complexity: a Modern Approach
i Computational Complexity: A Modern Approach Draft of a book: Dated January 2007 Comments welcome! Sanjeev Arora and Boaz Barak Princeton University [email protected] Not to be reproduced or distributed without the authors’ permission This is an Internet draft. Some chapters are more finished than others. References and attributions are very preliminary and we apologize in advance for any omissions (but hope you will nevertheless point them out to us). Please send us bugs, typos, missing references or general comments to [email protected] — Thank You!! DRAFT ii DRAFT Chapter 9 Complexity of counting “It is an empirical fact that for many combinatorial problems the detection of the existence of a solution is easy, yet no computationally efficient method is known for counting their number.... for a variety of problems this phenomenon can be explained.” L. Valiant 1979 The class NP captures the difficulty of finding certificates. However, in many contexts, one is interested not just in a single certificate, but actually counting the number of certificates. This chapter studies #P, (pronounced “sharp p”), a complexity class that captures this notion. Counting problems arise in diverse fields, often in situations having to do with estimations of probability. Examples include statistical estimation, statistical physics, network design, and more. Counting problems are also studied in a field of mathematics called enumerative combinatorics, which tries to obtain closed-form mathematical expressions for counting problems. To give an example, in the 19th century Kirchoff showed how to count the number of spanning trees in a graph using a simple determinant computation. Results in this chapter will show that for many natural counting problems, such efficiently computable expressions are unlikely to exist. -
Quantum Computer: Quantum Model and Reality
Quantum Computer: Quantum Model and Reality Vasil Penchev, [email protected] Bulgarian Academy of Sciences: Institute of Philosophy and Sociology: Dept. of Logical Systems and Models Abstract. Any computer can create a model of reality. The hypothesis that quantum computer can generate such a model designated as quantum, which coincides with the modeled reality, is discussed. Its reasons are the theorems about the absence of “hidden variables” in quantum mechanics. The quantum modeling requires the axiom of choice. The following conclusions are deduced from the hypothesis. A quantum model unlike a classical model can coincide with reality. Reality can be interpreted as a quantum computer. The physical processes represent computations of the quantum computer. Quantum information is the real fundament of the world. The conception of quantum computer unifies physics and mathematics and thus the material and the ideal world. Quantum computer is a non-Turing machine in principle. Any quantum computing can be interpreted as an infinite classical computational process of a Turing machine. Quantum computer introduces the notion of “actually infinite computational process”. The discussed hypothesis is consistent with all quantum mechanics. The conclusions address a form of neo-Pythagoreanism: Unifying the mathematical and physical, quantum computer is situated in an intermediate domain of their mutual transformations. Key words: model, quantum computer, reality, Turing machine Eight questions: There are a few most essential questions about the philosophical interpretation of quantum computer. They refer to the fundamental problems in ontology and epistemology rather than philosophy of science or that of information and computation only. The contemporary development of quantum mechanics and the theory of quantum information generate them. -
The Complexity Zoo
The Complexity Zoo Scott Aaronson www.ScottAaronson.com LATEX Translation by Chris Bourke [email protected] 417 classes and counting 1 Contents 1 About This Document 3 2 Introductory Essay 4 2.1 Recommended Further Reading ......................... 4 2.2 Other Theory Compendia ............................ 5 2.3 Errors? ....................................... 5 3 Pronunciation Guide 6 4 Complexity Classes 10 5 Special Zoo Exhibit: Classes of Quantum States and Probability Distribu- tions 110 6 Acknowledgements 116 7 Bibliography 117 2 1 About This Document What is this? Well its a PDF version of the website www.ComplexityZoo.com typeset in LATEX using the complexity package. Well, what’s that? The original Complexity Zoo is a website created by Scott Aaronson which contains a (more or less) comprehensive list of Complexity Classes studied in the area of theoretical computer science known as Computa- tional Complexity. I took on the (mostly painless, thank god for regular expressions) task of translating the Zoo’s HTML code to LATEX for two reasons. First, as a regular Zoo patron, I thought, “what better way to honor such an endeavor than to spruce up the cages a bit and typeset them all in beautiful LATEX.” Second, I thought it would be a perfect project to develop complexity, a LATEX pack- age I’ve created that defines commands to typeset (almost) all of the complexity classes you’ll find here (along with some handy options that allow you to conveniently change the fonts with a single option parameters). To get the package, visit my own home page at http://www.cse.unl.edu/~cbourke/. -
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA-Completeness of the Local Hamiltonian Problem
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA-completeness of the Local Hamiltonian problem Scribe: Jenish C. Mehta The Complexity Class BQP The complexity class BQP is the quantum analog of the class BPP. It consists of all languages that can be decided in quantum polynomial time. More formally, Definition 1. A language L 2 BQP if there exists a classical polynomial time algorithm A that ∗ maps inputs x 2 f0, 1g to quantum circuits Cx on n = poly(jxj) qubits, where the circuit is considered a sequence of unitary operators each on 2 qubits, i.e Cx = UTUT−1...U1 where each 2 2 Ui 2 L C ⊗ C , such that: 2 i. Completeness: x 2 L ) Pr(Cx accepts j0ni) ≥ 3 1 ii. Soundness: x 62 L ) Pr(Cx accepts j0ni) ≤ 3 We say that the circuit “Cx accepts jyi” if the first output qubit measured in Cxjyi is 0. More j0i specifically, letting P1 = j0ih0j1 be the projection of the first qubit on state j0i, j0i 2 Pr(Cx accepts jyi) =k (P1 ⊗ In−1)Cxjyi k2 The Complexity Class QMA The complexity class QMA (or BQNP, as Kitaev originally named it) is the quantum analog of the class NP. More formally, Definition 2. A language L 2 QMA if there exists a classical polynomial time algorithm A that ∗ maps inputs x 2 f0, 1g to quantum circuits Cx on n + q = poly(jxj) qubits, such that: 2q i. Completeness: x 2 L ) 9jyi 2 C , kjyik2 = 1, such that Pr(Cx accepts j0ni ⊗ 2 jyi) ≥ 3 2q 1 ii. -
Restricted Versions of the Two-Local Hamiltonian Problem
The Pennsylvania State University The Graduate School Eberly College of Science RESTRICTED VERSIONS OF THE TWO-LOCAL HAMILTONIAN PROBLEM A Dissertation in Physics by Sandeep Narayanaswami c 2013 Sandeep Narayanaswami Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy August 2013 The dissertation of Sandeep Narayanaswami was reviewed and approved* by the following: Sean Hallgren Associate Professor of Computer Science and Engineering Dissertation Adviser, Co-Chair of Committee Nitin Samarth Professor of Physics Head of the Department of Physics Co-Chair of Committee David S Weiss Professor of Physics Jason Morton Assistant Professor of Mathematics *Signatures are on file in the Graduate School. Abstract The Hamiltonian of a physical system is its energy operator and determines its dynamics. Un- derstanding the properties of the ground state is crucial to understanding the system. The Local Hamiltonian problem, being an extension of the classical Satisfiability problem, is thus a very well-motivated and natural problem, from both physics and computer science perspectives. In this dissertation, we seek to understand special cases of the Local Hamiltonian problem in terms of algorithms and computational complexity. iii Contents List of Tables vii List of Tables vii Acknowledgments ix 1 Introduction 1 2 Background 6 2.1 Classical Complexity . .6 2.2 Quantum Computation . .9 2.3 Generalizations of SAT . 11 2.3.1 The Ising model . 13 2.3.2 QMA-complete Local Hamiltonians . 13 2.3.3 Projection Hamiltonians, or Quantum k-SAT . 14 2.3.4 Commuting Local Hamiltonians . 14 2.3.5 Other special cases . 15 2.3.6 Approximation Algorithms and Heuristics . -
Complexity Theory
Complexity Theory Course Notes Sebastiaan A. Terwijn Radboud University Nijmegen Department of Mathematics P.O. Box 9010 6500 GL Nijmegen the Netherlands [email protected] Copyright c 2010 by Sebastiaan A. Terwijn Version: December 2017 ii Contents 1 Introduction 1 1.1 Complexity theory . .1 1.2 Preliminaries . .1 1.3 Turing machines . .2 1.4 Big O and small o .........................3 1.5 Logic . .3 1.6 Number theory . .4 1.7 Exercises . .5 2 Basics 6 2.1 Time and space bounds . .6 2.2 Inclusions between classes . .7 2.3 Hierarchy theorems . .8 2.4 Central complexity classes . 10 2.5 Problems from logic, algebra, and graph theory . 11 2.6 The Immerman-Szelepcs´enyi Theorem . 12 2.7 Exercises . 14 3 Reductions and completeness 16 3.1 Many-one reductions . 16 3.2 NP-complete problems . 18 3.3 More decision problems from logic . 19 3.4 Completeness of Hamilton path and TSP . 22 3.5 Exercises . 24 4 Relativized computation and the polynomial hierarchy 27 4.1 Relativized computation . 27 4.2 The Polynomial Hierarchy . 28 4.3 Relativization . 31 4.4 Exercises . 32 iii 5 Diagonalization 34 5.1 The Halting Problem . 34 5.2 Intermediate sets . 34 5.3 Oracle separations . 36 5.4 Many-one versus Turing reductions . 38 5.5 Sparse sets . 38 5.6 The Gap Theorem . 40 5.7 The Speed-Up Theorem . 41 5.8 Exercises . 43 6 Randomized computation 45 6.1 Probabilistic classes . 45 6.2 More about BPP . 48 6.3 The classes RP and ZPP . -
Interactive Proofs 1 1 Pspace ⊆ IP
CS294: Probabilistically Checkable and Interactive Proofs January 24, 2017 Interactive Proofs 1 Instructor: Alessandro Chiesa & Igor Shinkar Scribe: Mariel Supina 1 Pspace ⊆ IP The first proof that Pspace ⊆ IP is due to Shamir, and a simplified proof was given by Shen. These notes discuss the simplified version in [She92], though most of the ideas are the same as those in [Sha92]. Notes by Katz also served as a reference [Kat11]. Theorem 1 ([Sha92]) Pspace ⊆ IP. To show the inclusion of Pspace in IP, we need to begin with a Pspace-complete language. 1.1 True Quantified Boolean Formulas (tqbf) Definition 2 A quantified boolean formula (QBF) is an expression of the form 8x19x28x3 ::: 9xnφ(x1; : : : ; xn); (1) where φ is a boolean formula on n variables. Note that since each variable in a QBF is quantified, a QBF is either true or false. Definition 3 tqbf is the language of all boolean formulas φ such that if φ is a formula on n variables, then the corresponding QBF (1) is true. Fact 4 tqbf is Pspace-complete (see section 2 for a proof). Hence to show that Pspace ⊆ IP, it suffices to show that tqbf 2 IP. Claim 5 tqbf 2 IP. In order prove claim 5, we will need to present a complete and sound interactive protocol that decides whether a given QBF is true. In the sum-check protocol we used an arithmetization of a 3-CNF boolean formula. Likewise, here we will need a way to arithmetize a QBF. 1.2 Arithmetization of a QBF We begin with a boolean formula φ, and we let n be the number of variables and m the number of clauses of φ. -
Interactive Proofs for Quantum Computations
Innovations in Computer Science 2010 Interactive Proofs For Quantum Computations Dorit Aharonov Michael Ben-Or Elad Eban School of Computer Science, The Hebrew University of Jerusalem, Israel [email protected] [email protected] [email protected] Abstract: The widely held belief that BQP strictly contains BPP raises fundamental questions: Upcoming generations of quantum computers might already be too large to be simulated classically. Is it possible to experimentally test that these systems perform as they should, if we cannot efficiently compute predictions for their behavior? Vazirani has asked [21]: If computing predictions for Quantum Mechanics requires exponential resources, is Quantum Mechanics a falsifiable theory? In cryptographic settings, an untrusted future company wants to sell a quantum computer or perform a delegated quantum computation. Can the customer be convinced of correctness without the ability to compare results to predictions? To provide answers to these questions, we define Quantum Prover Interactive Proofs (QPIP). Whereas in standard Interactive Proofs [13] the prover is computationally unbounded, here our prover is in BQP, representing a quantum computer. The verifier models our current computational capabilities: it is a BPP machine, with access to few qubits. Our main theorem can be roughly stated as: ”Any language in BQP has a QPIP, and moreover, a fault tolerant one” (providing a partial answer to a challenge posted in [1]). We provide two proofs. The simpler one uses a new (possibly of independent interest) quantum authentication scheme (QAS) based on random Clifford elements. This QPIP however, is not fault tolerant. Our second protocol uses polynomial codes QAS due to Ben-Or, Cr´epeau, Gottesman, Hassidim, and Smith [8], combined with quantum fault tolerance and secure multiparty quantum computation techniques. -
Polynomial Hierarchy
CSE200 Lecture Notes – Polynomial Hierarchy Lecture by Russell Impagliazzo Notes by Jiawei Gao February 18, 2016 1 Polynomial Hierarchy Recall from last class that for language L, we defined PL is the class of problems poly-time Turing reducible to L. • NPL is the class of problems with witnesses verifiable in P L. • In other words, these problems can be considered as computed by deterministic or nonde- terministic TMs that can get access to an oracle machine for L. The polynomial hierarchy (or polynomial-time hierarchy) can be defined by a hierarchy of problems that have oracle access to the lower level problems. Definition 1 (Oracle definition of PH). Define classes P Σ1 = NP. P • P Σi For i 1, Σi 1 = NP . • ≥ + Symmetrically, define classes P Π1 = co-NP. • P ΠP For i 1, Π co-NP i . i+1 = • ≥ S P S P The Polynomial Hierarchy (PH) is defined as PH = i Σi = i Πi . 1.1 If P = NP, then PH collapses to P P Theorem 2. If P = NP, then P = Σi i. 8 Proof. By induction on i. P Base case: For i = 1, Σi = NP = P by definition. P P ΣP P Inductive step: Assume P NP and Σ P. Then Σ NP i NP P. = i = i+1 = = = 1 CSE 200 Winter 2016 P ΣP Figure 1: An overview of classes in PH. The arrows denote inclusion. Here ∆ P i . (Image i+1 = source: Wikipedia.) Similarly, if any two different levels in PH turn out to be the equal, then PH collapses to the lower of the two levels. -
The Polynomial Hierarchy and Alternations
Chapter 5 The Polynomial Hierarchy and Alternations “..synthesizing circuits is exceedingly difficulty. It is even more difficult to show that a circuit found in this way is the most economical one to realize a function. The difficulty springs from the large number of essentially different networks available.” Claude Shannon 1949 This chapter discusses the polynomial hierarchy, a generalization of P, NP and coNP that tends to crop up in many complexity theoretic inves- tigations (including several chapters of this book). We will provide three equivalent definitions for the polynomial hierarchy, using quantified pred- icates, alternating Turing machines, and oracle TMs (a fourth definition, using uniform families of circuits, will be given in Chapter 6). We also use the hierarchy to show that solving the SAT problem requires either linear space or super-linear time. p p 5.1 The classes Σ2 and Π2 To understand the need for going beyond nondeterminism, let’s recall an NP problem, INDSET, for which we do have a short certificate of membership: INDSET = {hG, ki : graph G has an independent set of size ≥ k} . Consider a slight modification to the above problem, namely, determin- ing the largest independent set in a graph (phrased as a decision problem): EXACT INDSET = {hG, ki : the largest independent set in G has size exactly k} . Web draft 2006-09-28 18:09 95 Complexity Theory: A Modern Approach. c 2006 Sanjeev Arora and Boaz Barak. DRAFTReferences and attributions are still incomplete. P P 96 5.1. THE CLASSES Σ2 AND Π2 Now there seems to be no short certificate for membership: hG, ki ∈ EXACT INDSET iff there exists an independent set of size k in G and every other independent set has size at most k. -
Distribution of Units of Real Quadratic Number Fields
Y.-M. J. Chen, Y. Kitaoka and J. Yu Nagoya Math. J. Vol. 158 (2000), 167{184 DISTRIBUTION OF UNITS OF REAL QUADRATIC NUMBER FIELDS YEN-MEI J. CHEN, YOSHIYUKI KITAOKA and JING YU1 Dedicated to the seventieth birthday of Professor Tomio Kubota Abstract. Let k be a real quadratic field and k, E the ring of integers and the group of units in k. Denoting by E( ¡ ) the subgroup represented by E of × ¡ ¡ ( k= ¡ ) for a prime ideal , we show that prime ideals for which the order of E( ¡ ) is theoretically maximal have a positive density under the Generalized Riemann Hypothesis. 1. Statement of the result x Let k be a real quadratic number field with discriminant D0 and fun- damental unit (> 1), and let ok and E be the ring of integers in k and the set of units in k, respectively. For a prime ideal p of k we denote by E(p) the subgroup of the unit group (ok=p)× of the residue class group modulo p con- sisting of classes represented by elements of E and set Ip := [(ok=p)× : E(p)], where p is the rational prime lying below p. It is obvious that Ip is inde- pendent of the choice of prime ideals lying above p. Set 1; if p is decomposable or ramified in k, ` := 8p 1; if p remains prime in k and N () = 1, p − k=Q <(p 1)=2; if p remains prime in k and N () = 1, − k=Q − : where Nk=Q stands for the norm from k to the rational number field Q. -
STRONGLY UNIVERSAL QUANTUM TURING MACHINES and INVARIANCE of KOLMOGOROV COMPLEXITY (AUGUST 11, 2007) 2 Such That the Aforementioned Halting Conditions Are Satisfied
STRONGLY UNIVERSAL QUANTUM TURING MACHINES AND INVARIANCE OF KOLMOGOROV COMPLEXITY (AUGUST 11, 2007) 1 Strongly Universal Quantum Turing Machines and Invariance of Kolmogorov Complexity Markus M¨uller Abstract—We show that there exists a universal quantum Tur- For a compact presentation of the results by Bernstein ing machine (UQTM) that can simulate every other QTM until and Vazirani, see the book by Gruska [4]. Additional rele- the other QTM has halted and then halt itself with probability one. vant literature includes Ozawa and Nishimura [5], who gave This extends work by Bernstein and Vazirani who have shown that there is a UQTM that can simulate every other QTM for necessary and sufficient conditions that a QTM’s transition an arbitrary, but preassigned number of time steps. function results in unitary time evolution. Benioff [6] has As a corollary to this result, we give a rigorous proof that worked out a slightly different definition which is based on quantum Kolmogorov complexity as defined by Berthiaume et a local Hamiltonian instead of a local transition amplitude. al. is invariant, i.e. depends on the choice of the UQTM only up to an additive constant. Our proof is based on a new mathematical framework for A. Quantum Turing Machines and their Halting Conditions QTMs, including a thorough analysis of their halting behaviour. Our discussion will rely on the definition by Bernstein and We introduce the notion of mutually orthogonal halting spaces and show that the information encoded in an input qubit string Vazirani. We describe their model in detail in Subsection II-B.