On AC0[⊕] and Variants of the Majority Function∗
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Randomised Computation 1 TM Taking Advices 2 Karp-Lipton Theorem
INFR11102: Computational Complexity 29/10/2019 Lecture 13: More on circuit models; Randomised Computation Lecturer: Heng Guo 1 TM taking advices An alternative way to characterize P=poly is via TMs that take advices. Definition 1. For functions F : N ! N and A : N ! N, the complexity class DTime[F ]=A consists of languages L such that there exist a TM with time bound F (n) and a sequence fangn2N of “advices” satisfying: • janj ≤ A(n); • for jxj = n, x 2 L if and only if M(x; an) = 1. The following theorem explains the notation P=poly, namely “polynomial-time with poly- nomial advice”. S c Theorem 1. P=poly = c;d2N DTime[n ]=nd . Proof. If L 2 P=poly, then it can be computed by a family C = fC1;C2; · · · g of Boolean circuits. Let an be the description of Cn, andS the polynomial time machine M just reads 2 c this description and simulates it. Hence L c;d2N DTime[n ]=nd . For the other direction, if a language L can be computed in polynomial-time with poly- nomial advice, say by TM M with advices fang, then we can construct circuits fDng to simulate M, as in the theorem P ⊂ P=poly in the last lecture. Hence, Dn(x; an) = 1 if and only if x 2 L. The final circuit Cn just does exactly what Dn does, except that Cn “hardwires” the advice an. Namely, Cn(x) := Dn(x; an). Hence, L 2 P=poly. 2 Karp-Lipton Theorem Dick Karp and Dick Lipton showed that NP is unlikely to be contained in P=poly [KL80]. -
On Uniformity Within NC
On Uniformity Within NC David A Mix Barrington Neil Immerman HowardStraubing University of Massachusetts University of Massachusetts Boston Col lege Journal of Computer and System Science Abstract In order to study circuit complexity classes within NC in a uniform setting we need a uniformity condition which is more restrictive than those in common use Twosuch conditions stricter than NC uniformity RuCo have app eared in recent research Immermans families of circuits dened by rstorder formulas ImaImb and a unifor mity corresp onding to Buss deterministic logtime reductions Bu We show that these two notions are equivalent leading to a natural notion of uniformity for lowlevel circuit complexity classes Weshow that recent results on the structure of NC Ba still hold true in this very uniform setting Finallyweinvestigate a parallel notion of uniformity still more restrictive based on the regular languages Here we givecharacterizations of sub classes of the regular languages based on their logical expressibility extending recentwork of Straubing Therien and Thomas STT A preliminary version of this work app eared as BIS Intro duction Circuit Complexity Computer scientists have long tried to classify problems dened as Bo olean predicates or functions by the size or depth of Bo olean circuits needed to solve them This eort has Former name David A Barrington Supp orted by NSF grant CCR Mailing address Dept of Computer and Information Science U of Mass Amherst MA USA Supp orted by NSF grants DCR and CCR Mailing address Dept of -
On the NP-Completeness of the Minimum Circuit Size Problem
On the NP-Completeness of the Minimum Circuit Size Problem John M. Hitchcock∗ A. Pavany Department of Computer Science Department of Computer Science University of Wyoming Iowa State University Abstract We study the Minimum Circuit Size Problem (MCSP): given the truth-table of a Boolean function f and a number k, does there exist a Boolean circuit of size at most k computing f? This is a fundamental NP problem that is not known to be NP-complete. Previous work has studied consequences of the NP-completeness of MCSP. We extend this work and consider whether MCSP may be complete for NP under more powerful reductions. We also show that NP-completeness of MCSP allows for amplification of circuit complexity. We show the following results. • If MCSP is NP-complete via many-one reductions, the following circuit complexity amplifi- Ω(1) cation result holds: If NP\co-NP requires 2n -size circuits, then ENP requires 2Ω(n)-size circuits. • If MCSP is NP-complete under truth-table reductions, then EXP 6= NP \ SIZE(2n ) for some > 0 and EXP 6= ZPP. This result extends to polylog Turing reductions. 1 Introduction Many natural NP problems are known to be NP-complete. Ladner's theorem [14] tells us that if P is different from NP, then there are NP-intermediate problems: problems that are in NP, not in P, but also not NP-complete. The examples arising out of Ladner's theorem come from diagonalization and are not natural. A canonical candidate example of a natural NP-intermediate problem is the Graph Isomorphism (GI) problem. -
Week 1: an Overview of Circuit Complexity 1 Welcome 2
Topics in Circuit Complexity (CS354, Fall’11) Week 1: An Overview of Circuit Complexity Lecture Notes for 9/27 and 9/29 Ryan Williams 1 Welcome The area of circuit complexity has a long history, starting in the 1940’s. It is full of open problems and frontiers that seem insurmountable, yet the literature on circuit complexity is fairly large. There is much that we do know, although it is scattered across several textbooks and academic papers. I think now is a good time to look again at circuit complexity with fresh eyes, and try to see what can be done. 2 Preliminaries An n-bit Boolean function has domain f0; 1gn and co-domain f0; 1g. At a high level, the basic question asked in circuit complexity is: given a collection of “simple functions” and a target Boolean function f, how efficiently can f be computed (on all inputs) using the simple functions? Of course, efficiency can be measured in many ways. The most natural measure is that of the “size” of computation: how many copies of these simple functions are necessary to compute f? Let B be a set of Boolean functions, which we call a basis set. The fan-in of a function g 2 B is the number of inputs that g takes. (Typical choices are fan-in 2, or unbounded fan-in, meaning that g can take any number of inputs.) We define a circuit C with n inputs and size s over a basis B, as follows. C consists of a directed acyclic graph (DAG) of s + n + 2 nodes, with n sources and one sink (the sth node in some fixed topological order on the nodes). -
Lecture 10: Learning DNF, AC0, Juntas Feb 15, 2007 Lecturer: Ryan O’Donnell Scribe: Elaine Shi
Analysis of Boolean Functions (CMU 18-859S, Spring 2007) Lecture 10: Learning DNF, AC0, Juntas Feb 15, 2007 Lecturer: Ryan O’Donnell Scribe: Elaine Shi 1 Learning DNF in Almost Polynomial Time From previous lectures, we have learned that if a function f is ǫ-concentrated on some collection , then we can learn the function using membership queries in poly( , 1/ǫ)poly(n) log(1/δ) time.S |S| O( w ) In the last lecture, we showed that a DNF of width w is ǫ-concentrated on a set of size n ǫ , and O( w ) concluded that width-w DNFs are learnable in time n ǫ . Today, we shall improve this bound, by showing that a DNF of width w is ǫ-concentrated on O(w log 1 ) a collection of size w ǫ . We shall hence conclude that poly(n)-size DNFs are learnable in almost polynomial time. Recall that in the last lecture we introduced H˚astad’s Switching Lemma, and we showed that 1 DNFs of width w are ǫ-concentrated on degrees up to O(w log ǫ ). Theorem 1.1 (Hastad’s˚ Switching Lemma) Let f be computable by a width-w DNF, If (I, X) is a random restriction with -probability ρ, then d N, ∗ ∀ ∈ d Pr[DT-depth(fX→I) >d] (5ρw) I,X ≤ Theorem 1.2 If f is a width-w DNF, then f(U)2 ǫ ≤ |U|≥OX(w log 1 ) ǫ b O(w log 1 ) To show that a DNF of width w is ǫ-concentrated on a collection of size w ǫ , we also need the following theorem: Theorem 1.3 If f is a width-w DNF, then 1 |U| f(U) 2 20w | | ≤ XU b Proof: Let (I, X) be a random restriction with -probability 1 . -
A Short History of Computational Complexity
The Computational Complexity Column by Lance FORTNOW NEC Laboratories America 4 Independence Way, Princeton, NJ 08540, USA [email protected] http://www.neci.nj.nec.com/homepages/fortnow/beatcs Every third year the Conference on Computational Complexity is held in Europe and this summer the University of Aarhus (Denmark) will host the meeting July 7-10. More details at the conference web page http://www.computationalcomplexity.org This month we present a historical view of computational complexity written by Steve Homer and myself. This is a preliminary version of a chapter to be included in an upcoming North-Holland Handbook of the History of Mathematical Logic edited by Dirk van Dalen, John Dawson and Aki Kanamori. A Short History of Computational Complexity Lance Fortnow1 Steve Homer2 NEC Research Institute Computer Science Department 4 Independence Way Boston University Princeton, NJ 08540 111 Cummington Street Boston, MA 02215 1 Introduction It all started with a machine. In 1936, Turing developed his theoretical com- putational model. He based his model on how he perceived mathematicians think. As digital computers were developed in the 40's and 50's, the Turing machine proved itself as the right theoretical model for computation. Quickly though we discovered that the basic Turing machine model fails to account for the amount of time or memory needed by a computer, a critical issue today but even more so in those early days of computing. The key idea to measure time and space as a function of the length of the input came in the early 1960's by Hartmanis and Stearns. -
BQP and the Polynomial Hierarchy 1 Introduction
BQP and The Polynomial Hierarchy based on `BQP and The Polynomial Hierarchy' by Scott Aaronson Deepak Sirone J., 17111013 Hemant Kumar, 17111018 Dept. of Computer Science and Engineering Dept. of Computer Science and Engineering Indian Institute of Technology Kanpur Indian Institute of Technology Kanpur Abstract The problem of comparing two complexity classes boils down to either finding a problem which can be solved using the resources of one class but cannot be solved in the other thereby showing they are different or showing that the resources needed by one class can be simulated within the resources of the other class and hence implying a containment. When the relation between the resources provided by two classes such as the classes BQP and PH is not well known, researchers try to separate the classes in the oracle query model as the first step. This paper tries to break the ice about the relationship between BQP and PH, which has been open for a long time by presenting evidence that quantum computers can solve problems outside of the polynomial hierarchy. The first result shows that there exists a relation problem which is solvable in BQP, but not in PH, with respect to an oracle. Thus gives evidence of separation between BQP and PH. The second result shows an oracle relation problem separating BQP from BPPpath and SZK. 1 Introduction The problem of comparing the complexity classes BQP and the polynomial heirarchy has been identified as one of the grand challenges of the field. The paper \BQP and the Polynomial Heirarchy" by Scott Aaronson proves an oracle separation result for BQP and the polynomial heirarchy in the form of two main results: A 1. -
Multiparty Communication Complexity and Threshold Circuit Size of AC^0
2009 50th Annual IEEE Symposium on Foundations of Computer Science Multiparty Communication Complexity and Threshold Circuit Size of AC0 Paul Beame∗ Dang-Trinh Huynh-Ngoc∗y Computer Science and Engineering Computer Science and Engineering University of Washington University of Washington Seattle, WA 98195-2350 Seattle, WA 98195-2350 [email protected] [email protected] Abstract— We prove an nΩ(1)=4k lower bound on the random- that the Generalized Inner Product function in ACC0 requires ized k-party communication complexity of depth 4 AC0 functions k-party NOF communication complexity Ω(n=4k) which is in the number-on-forehead (NOF) model for up to Θ(log n) polynomial in n for k up to Θ(log n). players. These are the first non-trivial lower bounds for general 0 NOF multiparty communication complexity for any AC0 function However, for AC functions much less has been known. for !(log log n) players. For non-constant k the bounds are larger For the communication complexity of the set disjointness than all previous lower bounds for any AC0 function even for function with k players (which is in AC0) there are lower simultaneous communication complexity. bounds of the form Ω(n1=(k−1)=(k−1)) in the simultaneous Our lower bounds imply the first superpolynomial lower bounds NOF [24], [5] and nΩ(1=k)=kO(k) in the one-way NOF for the simulation of AC0 by MAJ ◦ SYMM ◦ AND circuits, showing that the well-known quasipolynomial simulations of AC0 model [26]. These are sub-polynomial lower bounds for all by such circuits are qualitatively optimal, even for formulas of non-constant values of k and, at best, polylogarithmic when small constant depth. -
NP-Complete Problems and Physical Reality
NP-complete Problems and Physical Reality Scott Aaronson∗ Abstract Can NP-complete problems be solved efficiently in the physical universe? I survey proposals including soap bubbles, protein folding, quantum computing, quantum advice, quantum adia- batic algorithms, quantum-mechanical nonlinearities, hidden variables, relativistic time dilation, analog computing, Malament-Hogarth spacetimes, quantum gravity, closed timelike curves, and “anthropic computing.” The section on soap bubbles even includes some “experimental” re- sults. While I do not believe that any of the proposals will let us solve NP-complete problems efficiently, I argue that by studying them, we can learn something not only about computation but also about physics. 1 Introduction “Let a computer smear—with the right kind of quantum randomness—and you create, in effect, a ‘parallel’ machine with an astronomical number of processors . All you have to do is be sure that when you collapse the system, you choose the version that happened to find the needle in the mathematical haystack.” —From Quarantine [31], a 1992 science-fiction novel by Greg Egan If I had to debate the science writer John Horgan’s claim that basic science is coming to an end [48], my argument would lean heavily on one fact: it has been only a decade since we learned that quantum computers could factor integers in polynomial time. In my (unbiased) opinion, the showdown that quantum computing has forced—between our deepest intuitions about computers on the one hand, and our best-confirmed theory of the physical world on the other—constitutes one of the most exciting scientific dramas of our time. -
0.1 Axt, Loop Program, and Grzegorczyk Hier- Archies
1 0.1 Axt, Loop Program, and Grzegorczyk Hier- archies Computable functions can have some quite complex definitions. For example, a loop programmable function might be given via a loop program that has depth of nesting of the loop-end pair, say, equal to 200. Now this is complex! Or a function might be given via an arbitrarily complex sequence of primitive recursions, with the restriction that the computed function is majorized by some known function, for all values of the input (for the concept of majorization see Subsection on the Ackermann function.). But does such definitional|and therefore, \static"|complexity have any bearing on the computational|dynamic|complexity of the function? We will see that it does, and we will connect definitional and computational complexities quantitatively. Our study will be restricted to the class PR that we will subdivide into an infinite sequence of increasingly more inclusive subclasses, Si. A so-called hierarchy of classes of functions. 0.1.0.1 Definition. A sequence (Si)i≥0 of subsets of PR is a primitive recur- sive hierarchy provided all of the following hold: (1) Si ⊆ Si+1, for all i ≥ 0 S (2) PR = i≥0 Si. The hierarchy is proper or nontrivial iff Si 6= Si+1, for all but finitely many i. If f 2 Si then we say that its level in the hierarchy is ≤ i. If f 2 Si+1 − Si, then its level is equal to i + 1. The first hierarchy that we will define is due to Axt and Heinermann [[5] and [1]]. -
Verifying Proofs in Constant Depth
This is a repository copy of Verifying proofs in constant depth. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/74775/ Proceedings Paper: Beyersdorff, O, Vollmer, H, Datta, S et al. (4 more authors) (2011) Verifying proofs in constant depth. In: Proceedings MFCS 2011. Mathematical Foundations of Computer Science 2011, 22 - 26 August 2011, Warsaw, Poland. Springer Verlag , 84 - 95 . ISBN 978-3-642-22992-3 https://doi.org/10.1007/978-3-642-22993-0_11 Reuse See Attached Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request. [email protected] https://eprints.whiterose.ac.uk/ Verifying Proofs in Constant Depth∗ Olaf Beyersdorff1, Samir Datta2, Meena Mahajan3, Gido Scharfenberger-Fabian4, Karteek Sreenivasaiah3, Michael Thomas1, and Heribert Vollmer1 1 Institut f¨ur Theoretische Informatik, Leibniz Universit¨at Hannover, Germany 2 Chennai Mathematical Institute, India 3 Institute of Mathematical Sciences, Chennai, India 4 Institut f¨ur Mathematik und Informatik, Ernst-Moritz-Arndt-Universit¨at Greifswald, Germany Abstract. In this paper we initiate the study of proof systems where verification of proofs proceeds by NC0 circuits. We investigate the ques- tion which languages admit proof systems in this very restricted model. Formulated alternatively, we ask which languages can be enumerated by NC0 functions. Our results show that the answer to this problem is not determined by the complexity of the language. On the one hand, we con- struct NC0 proof systems for a variety of languages ranging from regular to NP-complete. -
Quantum Computational Complexity Theory Is to Un- Derstand the Implications of Quantum Physics to Computational Complexity Theory
Quantum Computational Complexity John Watrous Institute for Quantum Computing and School of Computer Science University of Waterloo, Waterloo, Ontario, Canada. Article outline I. Definition of the subject and its importance II. Introduction III. The quantum circuit model IV. Polynomial-time quantum computations V. Quantum proofs VI. Quantum interactive proof systems VII. Other selected notions in quantum complexity VIII. Future directions IX. References Glossary Quantum circuit. A quantum circuit is an acyclic network of quantum gates connected by wires: the gates represent quantum operations and the wires represent the qubits on which these operations are performed. The quantum circuit model is the most commonly studied model of quantum computation. Quantum complexity class. A quantum complexity class is a collection of computational problems that are solvable by a cho- sen quantum computational model that obeys certain resource constraints. For example, BQP is the quantum complexity class of all decision problems that can be solved in polynomial time by a arXiv:0804.3401v1 [quant-ph] 21 Apr 2008 quantum computer. Quantum proof. A quantum proof is a quantum state that plays the role of a witness or certificate to a quan- tum computer that runs a verification procedure. The quantum complexity class QMA is defined by this notion: it includes all decision problems whose yes-instances are efficiently verifiable by means of quantum proofs. Quantum interactive proof system. A quantum interactive proof system is an interaction between a verifier and one or more provers, involving the processing and exchange of quantum information, whereby the provers attempt to convince the verifier of the answer to some computational problem.