Counter machine

A counter machine is an abstract machine used in formal logic and theoretical computer science to model computation. It is the most primitive of the four types of register machines. A counter machine comprises a set of one or more unbounded registers, each of which can hold a single non-negative integer, and a list of (usually sequential) arithmetic and control instructions for the machine to follow.

Basic features

For a given counter machine model the instruction set is tinyfrom just one to six or seven instructions. Most models contain a few arithmetic operations and at least one conditional operation (if condition is true, then jump). Three base models, each using three instructions, are drawn from the following collection. (The abbreviations are arbitrary.)

In addition, a machine usually has a HALT instruction, which stops the machine (normally after the result has been computed).

Using the instructions mentioned above, various authors have discussed certain counter machines:

The three counter machine base models have the same computational power since the instructions of one model can be derived from those of another. All are equivalent to the computational power of Turing machines (but only if Gödel numbers are used to encode data in the register or registers; otherwise their power is equivalent to the primitive recursive functions). Due to their unary processing style, counter machines are typically exponentially slower than comparable Turing machines.

Alternative names, alternative models

The counter machine models go by a number of different names that may help to distinguish them by their peculiarities. In the following the instruction "JZDEC ( r )" is a compound instruction that tests to see if a register r is empty; if so then jump to instruction Iz, else if not then DECrement the contents of r:

Formal definition

A counter machine consists of:

  1. Labeled unbounded integer-valued registers: a finite (or infinite in some models) set of registers r0 ... rn each of which can hold any single non-negative integer (0, 1, 2, ... - i.e. unbounded). The registers do their own arithmetic; there may or may not be one or more special registers e.g. "accumulator" (See Random access machine for more on this).
  2. A state register that stores/identifies the current instruction to be executed. This register is finite and separate from the registers above; thus the counter machine model is an example of the Harvard architecture
  3. List of labelled, sequential instructions: A finite list of instructions I0 ... Im. The program store (instructions of the finite state machine) is not in the same physical "space" as the registers. Usually, but not always, like computer programs the instructions are listed in sequential order; unless a jump is successful, the default sequence continues in numerical order. Each of the instructions in the list is from a (very) small set, but this set does not include indirection. Historically most models drew their instructions from this set:
{ Increment (r), Decrement (r), Clear (r); Copy (rj,rk), conditional Jump if contents of r=0, conditional Jump if rj=rk, unconditional Jump, HALT }
Some models have either further atomized some of the above into no-parameter instructions, or combined them into a single instruction such as "Decrement" preceded by conditional jump-if-zero "JZ ( r, z )" . The atomization of instructions or the inclusion of convenience instructions causes no change in conceptual power, as any program in one variant can be straightforwardly translated to the other.
Alternative instruction-sets are discussed in the supplement Register machine models.

Example: COPY the count from register #2 to #3

This example shows how to create three more useful instructions: clear, unconditional jump, and copy.

The basic set (1) is used as defined here:

Instruction Effect on register "j" Effect on Instruction Counter Register ICR Summary
INC ( j ) [j] +1 → j [IC] +1 → IC Increment contents of register j; next instruction
DEC ( j ) [j] -1 → j [IC] +1 → IC Decrement contents of register j; next instruction
JZ ( j, z) IF [j] = 0 THEN Iz → IC ELSE [IC] +1 → IC If contents of register j=0 then instruction z else next instruction
HALT

Initial conditions:

Initially, register #2 contains "2". Registers #0, #1 and #3 are empty (contain "0"). Register #0 remains unchanged throughout calculations because it is used for the unconditional jump. Register #1 is a scratch pad. The program begins with instruction 1.

Final conditions:

The program HALTs with the contents of register #2 at its original count and the contents of register #3 equal to the original contents of register #2, i.e.,

[2] = [3].

Program High-level Description:

The program COPY ( #2, #3) has two parts. In the first part the program moves the contents of source register #2 to both scratch-pad #1 and to destination register #3; thus #1 and #3 will be copies of one another and of the original count in #2, but #2 is cleared in the process of decrementing it to zero. Unconditional jumps J (z) are done by tests of register #0, which always contains the number 0:

[#2] →#3; [#2] →#1; 0 →#2

In the second the part the program moves (returns, restores) the contents of scratch-pad #1 back to #2, clearing the scratch-pad #1 in the process:

[#1] →#2; 0 →#1

Program: The program, highlighted in yellow, is shown written left-to-right in the upper right.

A "run" of the program is shown below. Time runs down the page. The instructions are in yellow, the registers in blue. The program is flipped 90 degrees, with the instruction numbers (addresses) along the top, the instruction mnemonics under the addresses, and the instruction parameters under the mnemonics (one per cell):

1 2 3 4 5 6 7 8 9 10 ← Instruction number (address)
JZ DEC INC INC JZ JZ DEC INC JZ H ← Instruction
2 2 3 1 0 1 1 2 0 ← Register number
6 1 10 6 ← Jump-to instruction number
step IC Inst # reg # J-addr reg0 reg1 reg2 reg3 reg4 IC
start 0 0 2 0 0 1 move [#2] to #1 and #3:
1 1 JZ 2 6 0 0 2 0 0 1→2 JZ Jump fails: register #2 contains 2
2 2 DEC 2 0 0 0 2→1 0 0 2→3 DEC Decrement register #2 from 2 to 1
3 3 INC 3 0 0 0 1 0→1 0 3→4 INC Increment register #3 from 0 to 1
4 4 INC 1 0 0 0→1 1 1 0 4→5 INC Increment register #1 from 0 to 1
5 5 JZ 0 1 0 1 1 1 0 5→1 JZ U-Jump: register #0 is empty
6 1 JZ 2 6 0 1 1 1 0 1→2 JZ Jump fails: register #2 contains 1
7 2 DEC 2 0 0 1 1→0 1 0 2→3 DEC Decrement register #2 from 1 to 0
8 3 INC 3 0 0 1 0 1→2 0 3→4 INC Increment register #3 from 1 to 2
9 4 INC 1 0 0 1→2 0 2 0 4→5 INC Increment register #1 from 1 to 2
10 5 JZ 0 1 0 2 0 2 0 5→1 JZ U-Jump: register #0 is empty
11 1 JZ 2 6 0 2 0 2 0 1→6 JZ Jump !: register #2 is empty
move [1] to 2:
12 6 JZ 1 10 0 2 0 2 0 6→7 JZ Jump fails: register #1 contains 2
13 7 DEC 1 0 0 2→1 0 2 0 7→8 DEC Decrement register #1 from 2 to 1
14 8 INC 2 0 0 1 0→1 2 0 8→9 INC Increment register #2 from 0 to 1
15 9 JZ 0 6 0 1 1 2 0 9→6 JZ U-Jump: register #0 is empty
16 6 JZ 1 10 0 1 1 2 0 6→7 JZ Jump fails: register #1 contains 1
17 7 DEC 1 0 0 1→0 1 2 0 7→8 DEC Decrement register #1 from 1 to 0
18 8 INC 2 0 0 0 1→2 2 0 8→9 INC Increment register #2 from 1 to 2
19 9 JZ 0 6 0 0 2 2 0 9→6 JZ U-Jump: register #0 is empty
20 6 JZ 1 10 0 0 2 2 0 6→10 JZ Jump !: register #1 is empty
21 10 H 0 0 0 0 2 2 0 10→10 H HALT

The partial recursive functions: building "convenience instructions" using recursion

The example above demonstrates how the first basic instructions { INC, DEC, JZ } can create three more instructions—unconditional jump J, CLR, CPY. In a sense CPY used both CLR and J plus the base set. If register #3 had had contents initially, the sum of contents of #2 and #3 would have ended up in #3. So to be fully accurate CPY program should have preceded its moves with CLR (1) and CLR (2).

However, we do see that ADD would have been possible, easily. And in fact the following is summary of how the primitive recursive functions such as ADD, MULtiply and EXPonent can come about (see Boolos-Burgess-Jeffrey (2002) p. 45-51).

{ J, DEC, INC, JZ, H }
{ CLR, J, DEC, INC, JZ, H }
{ CPY, CLR, J, DEC, INC, JZ, H }
The above is the instruction set of Shepherdson-Sturgis (1963).
{ ADD, CPY, CLR, J, DEC, INC, JZ, H }
{ MUL, ADD, CPY, CLR, J, DEC, INC, JZ, H }
{ EXP, MUL, ADD, CPY, CLR, J, DEC, INC, JZ, H }

In general, we can build any partial- or total- primitive recursive function that we wish, by using the same methods. Indeed, Minsky (1967), Shepherdson-Sturgis (1963) and Boolos-Burgess-Jeffrey (2002) give demonstrations of how to form the five primitive recursive function "operators" (1-5 below) from the base set (1).

But what about full Turing equivalence? We need to add the sixth operator—the μ operator—to obtain the full equivalence, capable of creating the total- and partial- recursive functions:

  1. Zero function (or constant function)
  2. Successor function
  3. Identity function
  4. Composition function
  5. Primitive recursion (induction)
  6. μ operator (unbounded search operator)

The authors show that this is done easily within any of the available base sets (1, 2, or 3) (an example can be found at μ operator ). However, the reader needs to be cautioned that, even though the μ operator is easily created by the base instruction set doesn't mean that an arbitrary partial recursive function can be easily created with a base model -- Turing equivalence and partial recursive functions imply an unbounded μ operator, one that can scurry to the ends of the register chain ad infinitum searching for its goal. The problem is: registers must be called out explicily by number/name e.g. INC (47,528) and DEC (39,347) and this will exhaust the finite state machine's TABLE of instructions. No matter how "big" the finite state machine is, we can find a function that uses a "bigger" number of registers.

Problems with the counter machine model

The problems are discussed in detail in the article Random access machine. The problems fall into two major classes and a third "inconvenience" class:

(1) Unbounded capacities of registers versus bounded capacities of state-machine instructions: How will the machine create constants larger than the capacity of its finite state machine?

(2) Unbounded numbers of registers versus bounded numbers of state-machine instructions: How will the machine access registers with address-numbers beyond the reach/capability of its finite state machine?

(3) The fully reduced models are cumbersome:

Shepherdson and Sturgis (1963) are unapologetic about their 6-instruction set. They have made their choice based on "ease of programming... rather than economy" (p. 219 footnote 1).

Shepherdson and Sturgis' instructions ( [r] indicates "contents of register r"):

Minsky (1967) expanded his 2-instruction set { INC (z), JZDEC (r, Iz) } to { CLR (r), INC (r), JZDEC (r, Iz), J (Iz) } before his proof that a "Universal Program Machine" can be built with only two registers (p. 255ff).

Two-counter machines are Turing equivalent (with a caveat)

For every Turing machine, there is a 2CM that simulates it, given that the 2CM's input and output are properly encoded. This is proved in Minsky's book (Computation, 1967, p. 255-258), and an alternative proof is sketched below in three steps. First, a Turing machine can be simulated by a finite-state machine (FSM) equipped with two stacks. Then, two stacks can be simulated by four counters. Finally, four counters can be simulated by two counters.

Step 1: A Turing machine can be simulated by two stacks.

A Turing machine consists of an FSM and an infinite tape, initially filled with zeros, upon which the machine can write ones and zeros. At any time, the read/write head of the machine points to one cell on the tape. This tape can be conceptually cut in half at that point. Each half of the tape can be treated as a stack, where the top is the cell nearest the read/write head, and the bottom is some distance away from the head, with all zeros on the tape beyond the bottom. Accordingly, a Turing machine can be simulated by an FSM plus two stacks. Moving the head left or right is equivalent to popping a bit from one stack and pushing it onto the other. Writing is equivalent to changing the bit before pushing it.

Step 2: A stack can be simulated by two counters.

A stack containing zeros and ones can be simulated by two counters when the bits on the stack are thought of as representing a binary number (the topmost bit on the stack being the least significant bit). Pushing a zero onto the stack is equivalent to doubling the number. Pushing a one is equivalent to doubling and adding 1. Popping is equivalent to dividing by 2, where the remainder is the bit that was popped. Two counters can simulate this stack, in which one of the counters holds a number whose binary representation represents the bits on the stack, and the other counter is used as a scratchpad. To double the number in the first counter, the FSM can initialize the second counter to zero, then repeatedly decrement the first counter once and increment the second counter twice. This continues until the first counter reaches zero. At that point, the second counter will hold the doubled number. Halving is performed by decrementing one counter twice and increment the other once, and repeating until the first counter reaches zero. The remainder can be determined by whether it reached zero after an even or an odd number of steps, where the parity of the number of steps is encoded in the state of the FSM.

Step 3: Four counters can be simulated by two counters.

As before, one of the counters is used as scratchpad. The other holds an integer whose prime factorization is 2a3b5c7d. The exponents a, b, c, and d can be thought of as four virtual counters that are being packed (via Gödel numbering) into a single real counter. If the real counter is set to zero then incremented once, that is equivalent to setting all the virtual counters to zero. If the real counter is doubled, that is equivalent to incrementing a, and if it's halved, that's equivalent to decrementing a. By a similar procedure, it can be multiplied or divided by 3, which is equivalent to incrementing or decrementing b. Similarly, c and d can be incremented or decremented. To check if a virtual counter such as c is equal to zero, just divide the real counter by 5, see what the remainder is, then multiply by 5 and add back the remainder. That leaves the real counter unchanged. The remainder will have been nonzero if and only if c was zero.

As a result, an FSM with two counters can simulate four counters, which are in turn simulating two stacks, which are simulating a Turing machine. Therefore, an FSM plus two counters is at least as powerful as a Turing machine. A Turing machine can easily simulate an FSM with two counters, therefore the two machines have equivalent power.

The caveat: *If* its counters are initialised to N and 0, then a 2CM cannot calculate 2N

This result, together with a list of other functions of N that are not calculable by a two-counter machine when initialised with N in one counter and 0 in the other such as N2, sqrt(N), log2(N), etc., appears in a paper by Schroeppel (1972). The result is not surprising, because the two-counter machine model was proved (by Minsky) to be universal only when the argument N is appropriately encoded (by Gödelization) to simulate a Turing machine whose initial tape contains N encoded in unary; moreover, the output of the two-counter machine will be similarly encoded. This phenomenon is typical of very small bases of computation whose universality is proved only by simulation (e.g., many Turing tarpits, the smallest-known universal Turing machines, etc.).

The proof is preceded by some interesting theorems:

With regard to the second theorem that "A 3CM can compute any partial recursive function" the author challenges the reader with a "Hard Problem: Multiply two numbers using ony three counters" (p. 2). The main proof involves the notion that two-counter machines cannot compute arithmetic sequences with non-linear growth rates (p. 15) i.e. "the function 2X grows more rapidly than any arithmetic progression." (p. 11).

See also

References

    Jan van Leeuwen, ed. "Handbbook of Theoretical Computer Science. Volume A: Algorithms and Complexity, The MIT PRESS/Elsevier, 1990. ISBN 0-444-88071-2 (volume A). QA 76.H279 1990.
    van Emde Boas' treatment of SMMs appears on pp. 32-35. This treatment clarifies Schōnhage 1980 -- it closely follows but expands slightly the Schōnhage treatment. Both references may be needed for effective understanding.

    External links

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