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N-Dimensional Tensor Reversal

Updated 2 December 2025
  • N-dimensional tensor reversal is a technique that inverts tensor indices along each axis to achieve complete in-place reversal of multidimensional data.
  • The 2^n+1 algorithm efficiently performs cyclic rotation by partitioning the tensor into binary-indexed blocks using O(1) auxiliary space and linear time complexity.
  • This method underpins various applications such as data augmentation, scientific simulations, and optimized multidimensional array manipulation.

N-dimensional tensor reversal refers to the in-place rearrangement of elements within an nn-dimensional tensor according to an axis-reversal operation or to effect a cyclic shift (rotation) by a prescribed vector. This operation is foundational for array manipulation algorithms, including multidimensional data rotation, data augmentation, and low-level scientific computing routines. Achieving this task using O(1)O(1) auxiliary space and with time complexity linear in the number of tensor elements represents a significant algorithmic challenge, especially for high-dimensional data structures. An O(1)O(1) space, 2n+12^n+1 reversal algorithm for in-place nn-dimensional tensor rotation establishes a systematic generalization of the classical three-reversal method for arrays to arbitrary tensor order, grounded in recursive block-wise permutation and inversion properties (Chen, 27 Nov 2025).

1. Formal Definition and Properties of N-Dimensional Tensor Reversal

Given a tensor TT of order nn with shape (d0,d1,,dn1)(d_0, d_1, \ldots, d_{n-1}) and multi-index i=(i0,,in1)\mathbf{i} = (i_0, \ldots, i_{n-1}) where 0i<d0 \le i_\ell < d_\ell, the nn-dimensional reversal operator Rev\mathit{Rev} is defined as: (Rev(T))i0,,in1=Td01i0,d11i1,,dn11in1.\bigl(\mathit{Rev}(T)\bigr)_{i_0,\ldots,i_{n-1}} = T_{d_0-1-i_0,\, d_1-1-i_1,\,\ldots,\, d_{n-1}-1-i_{n-1}}. This operator negates each per-axis index with respect to the axis range. Equivalently, for start and end vectors s=(0,,0)\mathbf{s} = (0,\ldots,0), e=(d01,,dn11)\mathbf{e}= (d_0-1, \ldots, d_{n-1}-1),

(Rev(T))i=Ts+ei.\bigl(\mathit{Rev}(T)\bigr)_{\mathbf{i}} = T_{\mathbf{s} + \mathbf{e} - \mathbf{i}}.

A fundamental property is involution: RevRev=I,\mathit{Rev} \circ \mathit{Rev} = I, implying that applying the reversal operation twice restores the original tensor.

2. The 2n+12^n+1 Reversal Algorithm for In-Place Rotation

The tensor cyclic rotation problem is to shift all elements by an index vector k=(k0,,kn1)\mathbf{k} = (k_0, \ldots, k_{n-1}), modulo the size of each dimension. The 2n+12^n+1 reversal algorithm proceeds as follows:

  1. Normalization: Each kk_\ell is reduced modulo dd_\ell.
  2. Global Tensor Reversal: Invoke Rev\mathit{Rev} over the full tensor, interchanging each block labeled by a binary block index b{0,1}n\mathbf{b} \in \{0,1\}^n with its complement.
  3. Block-Wise Reversals: Enumerate all 2n2^n blocks—each corresponding to a binary vector b\mathbf{b} that selects, per axis, whether the index is less (0) or greater/equal (1) to kk_\ell. For each block, reverse the sub-tensor indexed by that range if it is non-empty.

The algorithm utilizes only O(n)O(n) auxiliary scalars (for index vectors and temporary counters) and achieves O(N)O(N) total data movement, where N=dN=\prod_\ell d_\ell.

Pseudocode

Sub-Tensor Reversal

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function ReverseND(T, s[0..n-1], e[0..n-1])
    i ← s
    loop
        j ← s + e − i
        if i lex≥ j then break
        swap T[i] and T[j]
        d ← n−1
        while d ≥ 0 do
            if i[d] < e[d] then
                i[d] ← i[d] + 1
                break
            else
                i[d] ← s[d]
                d ← d − 1
            end if
        end while
        if d < 0 then break
    end loop
end function

Rotation by Vector k\mathbf{k}

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function RotateND(T, k[0..n-1])
    n ← dimensionality of T
    d[ℓ] ← shape of T in dimension ℓ
    for ℓ in 0..n-1 do
        k[ℓ] ← k[ℓ] mod d[ℓ]
    end for
    s_global ← (0,0,…,0)
    e_global ← (d[0]-1, …, d[n-1]-1)
    ReverseND(T, s_global, e_global)
    for b in 0..(2^n−1) do
        for ℓ in 0..n-1 do
            if the ℓ-th bit of b is 0 then
                s_block[ℓ] ← 0;          e_block[ℓ] ← k[ℓ]−1
            else
                s_block[ℓ] ← k[ℓ];      e_block[ℓ] ← d[ℓ]−1
            end if
        end for
        if ∀ℓ: s_block[ℓ] ≤ e_block[ℓ] then
            ReverseND(T, s_block, e_block)
        end if
    end for
end function
(Chen, 27 Nov 2025)

3. Algorithmic Invariants and Correctness

The 2n+12^n+1 reversal algorithm exploits the involutive property of Rev\mathit{Rev} and recursive block decomposition. The set of all tensor index vectors is partitioned into 2n2^n blocks, each demarcated by comparisons to the corresponding kk_\ell. Under the global reversal, block b\mathbf{b} receives the element-wise reversed content of block bˉ\bar{\mathbf{b}} (bitwise complement). Each inner block reversal undoes this internal order, enabling data from block bˉ\bar{\mathbf{b}} to be efficiently mapped to block b\mathbf{b}—effecting a cyclic shift. Applying Rev\mathit{Rev} twice (via the full reversal and block reversal) ensures each datum's correct placement via the composability of the involutive operator: Rev(Rev(Bbˉ))=Bbˉ.\mathit{Rev}(\mathit{Rev}(B_{\bar{\mathbf{b}}})) = B_{\bar{\mathbf{b}}}. This satisfies the correct data movement corresponding to a kk-shift in all axes, implemented entirely in-place with only pairwise swaps.

4. Computational Complexity

Time and space complexity characteristics are determined by the linear cost of elementary reversals and the block decomposition structure. A single reversal of a block of cardinality NsubN_{\mathrm{sub}} requires O(Nsub)O(N_{\mathrm{sub}}) swaps. The global reversal and all 2n2^n block reversals collectively cover the tensor domain exactly, resulting in total work of O(N)O(N), where N==0n1dN = \prod_{\ell=0}^{n-1} d_\ell. The memory overhead comprises O(n)O(n) scalars for indices and counters, making auxiliary space O(1)O(1) under the data-size model—a critical property for large-scale or memory-constrained contexts.

5. Illustrative Cases Across Multiple Dimensions

The 2n+12^n+1 reversal framework generalizes naturally from classical one-dimensional rotations to higher-order arrays with analogous block structures.

Dimensionality (nn) Number of Reversals Block Decomposition
1 3 (21+12^1+1) 2 segments (A, B)
2 5 (22+12^2+1) 4 quadrants (B00,B01,B10,B11)(B_{00}, B_{01}, B_{10}, B_{11})
3 9 (23+12^3+1) 8 octants labeled by (b0b1b2)(b_0b_1b_2)
  • For n=1n=1, a vector rotated by kk is reversed globally, then both left and right segments are reversed in-place: [1234567]Rev[7654321][1\,2\,3\,4\,5\,6\,7] \xrightarrow{\mathit{Rev}} [7\,6\,5\,4\,3\,2\,1], then two segment reversals yield [5671234][5\,6\,7\,1\,2\,3\,4]—the desired rotation.
  • For n=2n=2, a d0×d1d_0 \times d_1 matrix is split at (k0,k1)(k_0, k_1) into quadrants, reversed globally, then each quadrant reversed, resulting in a (k0,k1)(k_0, k_1) block-wise cyclic permutation.
  • For n=3n=3, eight octants are manipulated analogously, with all blockwise mapping following bitwise complement labeling.

In each case, data in any block BbB_{\mathbf{b}} is mapped, via double reversal, into the location for a cyclic shift by k\mathbf{k}.

6. Applications and Context

N-dimensional tensor reversal and in-place cyclic rotation are central to array manipulation libraries, data augmentation pipelines, scientific simulations involving periodic boundaries, and bijective data reshaping. The O(1)O(1) space requirement is particularly relevant for devices with constrained memory or in high-throughput environments where allocation of large auxiliary workspace is infeasible. The method generalizes classical array and matrix reversal tools to higher-order data, preserving strict in-place semantics. When compared to alternative tensor permutation strategies involving auxiliary buffers, the 2n+12^n+1 reversal method minimizes temporal and spatial overhead.

7. Significance, Limitations, and Extensions

The 2n+12^n+1 reversal algorithm formalizes and unifies a family of in-place tensor cyclic permutation algorithms, extending the reach of elementary reversal-based methods to arbitrary dimension while optimizing for constant auxiliary space and linear time. Based on elementary index manipulations and swap operations, the approach is broadly applicable independent of the underlying data type or tensor storage layout, provided index arithmetic is feasible. A plausible implication is that further optimizations or parallel variants could extend this approach to distributed or multi-core hardware with care to avoid conflicting swaps and maintain in-place guarantees. The algorithm's dependence on 2n2^n block enumerations may render it less suitable for extremely high nn in practice, but for the most common cases (n6n \leq 6) its efficiency and robustness are particularly compelling (Chen, 27 Nov 2025).

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