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Holographic Knowledge Manifold (HKM)

Updated 4 July 2026
  • HKM is a manifold-based framework that represents knowledge using holographic embeddings and operators like circular correlation and FFT for efficient triple scoring.
  • It extends traditional knowledge-graph methods to include continual learning substrates with fractal quantization and holographic integration for large language models.
  • HKM also spans microscopic models and Riemannian semantic maps, providing diverse applications in memory theory and semantic literature analysis.

Searching arXiv for the cited HKM-related papers and closely related work. Searching for "Holographic Embeddings of Knowledge Graphs" and related equivalence papers. Holographic Knowledge Manifold (HKM) denotes a family of geometric and computational formulations in which knowledge is represented as a distributed structure and accessed through holographic composition, reconstruction, or interference operators. In the knowledge-graph setting, HKM is instantiated by holographic embeddings in which entities and relations share a vector space and triples are modeled through circular correlation; in a closely related frequency-domain formulation, the same scoring behavior is realized by complex embeddings (Nickel et al., 2015, Trouillon et al., 2017). Later uses of the term extend HKM to a four-phase continual-learning substrate for LLMs, to a microscopic holography-inspired memory model with area-law capacity, and to a Riemannian semantic map of scientific literature with interpolation and geodesic analysis (Arndt, 3 Sep 2025, Dvali, 2018, Okabe et al., 4 Jun 2026). Taken together, these works suggest that HKM is best understood as an umbrella notion for manifold-structured knowledge representations equipped with explicit binding, retrieval, or navigation rules.

1. Terminological scope and principal formulations

Across the cited literature, HKM refers to related but non-identical constructions. The common thread is that knowledge is not treated as an unstructured parameter collection; it is organized in a manifold or manifold-like substrate whose algebra determines how facts are composed, retrieved, updated, or traversed.

Formulation Representation Main mechanism
HolE for knowledge graphs Entities and relations in Rd\mathbb{R}^d Circular correlation, FFT-based scoring
HolE–ComplEx equivalence Real-domain or complex-domain embeddings DFT mapping, conjugation-based trilinear score
Continual-learning HKM Hierarchical graph M=(V,E,L)M=(V,E,L) Probabilistic entanglement, fractal quantization, holographic attention, diffraction chipping
Microscopic holography-inspired HKM Gapless shell modes on SdS^d Criticality, area-law mode counting, memory burden
Riemannian literature manifold as HKM 2D semantic map with reconstruction operators SPH interpolation, GPR, pull-back metric, geodesics

In the original knowledge-graph usage, the defining feature is holographic compositionality: entity pairs are combined by circular correlation, producing fixed-width tuple representations while retaining rich pairwise interactions (Nickel et al., 2015). In the continual-learning usage, HKM becomes a structured “knowledge substrate” for LLMs, built and updated through four phases while maintaining retrievability and bounded growth (Arndt, 3 Sep 2025). In the microscopic model, holography appears as an area-law scaling of gapless memory modes and a load-dependent stabilization effect; in the literature-mapping framework, the holographic interpretation is a projection/reconstruction duality in which a 2D screen supports local recovery of high-dimensional semantic content (Dvali, 2018, Okabe et al., 4 Jun 2026).

This suggests that HKM is not a single canonical architecture. Rather, it names a recurrent design pattern: distributed knowledge is embedded into a structured space, and specialized operators govern composition, reconstruction, or transport within that space.

2. HolE as the canonical knowledge-graph HKM

The foundational HKM construction in machine learning is HolE, or holographic embeddings of knowledge graphs. HolE represents entities eiRde_i \in \mathbb{R}^d and relations rpRdr_p \in \mathbb{R}^d in a common vector space and composes subject–object pairs by circular correlation. For a,bRda,b \in \mathbb{R}^d,

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},

and circular convolution is

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.

These operators admit FFT-based implementations,

ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),

so computing either operator costs O(dlogd)O(d\log d) rather than the M=(V,E,L)M=(V,E,L)0 cost of explicit tensor products (Nickel et al., 2015).

HolE scores a triple M=(V,E,L)M=(V,E,L)1 by

M=(V,E,L)M=(V,E,L)2

with probabilistic interpretation

M=(V,E,L)M=(V,E,L)3

where M=(V,E,L)M=(V,E,L)4. The central intuition is that correlation compresses the tensor product’s pairwise interactions into M=(V,E,L)M=(V,E,L)5 partitions, preserving rich feature interactions while keeping the representation fixed-width. The construction is directly linked to holographic associative memory: in HRR, associations are stored by circular convolution and retrieved by circular correlation, with superposition allowing multiple bindings in the same memory trace. HolE adopts correlation as the compositional operator for pairs M=(V,E,L)M=(V,E,L)6, while convolution reappears naturally in the gradients, mirroring storage/retrieval duality (Nickel et al., 2015).

Several algebraic properties are essential. First, circular correlation is non-commutative, M=(V,E,L)M=(V,E,L)7, which is crucial for encoding asymmetric or directed relations. Second, it contains an explicit similarity term, M=(V,E,L)M=(V,E,L)8, so similarity between entity embeddings is directly present in the composed representation. These two properties distinguish HolE from simpler diagonal or translational models.

Training is formulated either as logistic loss with M=(V,E,L)M=(V,E,L)9 regularization,

SdS^d0

or as pairwise margin-based ranking over true triples SdS^d1 and corrupted negatives SdS^d2,

SdS^d3

The parameter derivatives are

SdS^d4

In practice, Stochastic Gradient Descent with AdaGrad works well; the reported experiments trained baselines and HolE with SGD+AdaGrad on the ranking loss, used embedding dimensions typically 150–200, and tuned the learning rate and margin on validation data (Nickel et al., 2015).

The manifold interpretation follows from this algebra. Entities SdS^d5 and relations SdS^d6 lie in a structured, circularly compositional manifold SdS^d7, whose geometry is induced by the loss and the holographic operators. Querying is described as moving from SdS^d8 to the composite point SdS^d9 and projecting along eiRde_i \in \mathbb{R}^d0 via a dot product. This interpretation is the original sense in which HolE realizes an HKM.

3. Frequency-domain equivalence, empirical performance, and practical trade-offs

A major refinement of the HolE-based HKM is the recognition that its score is equivalent, up to a constant factor, to the score used by ComplEx. HolE uses the exact scoring function

eiRde_i \in \mathbb{R}^d1

where circular correlation is computed by

eiRde_i \in \mathbb{R}^d2

ComplEx instead uses complex-valued embeddings and scores

eiRde_i \in \mathbb{R}^d3

Using the Fourier correlation theorem and Parseval’s theorem, HolE’s score can be written as

eiRde_i \in \mathbb{R}^d4

and under conjugate symmetry with an appropriate half-spectrum parameterization one obtains direct proportionality:

eiRde_i \in \mathbb{R}^d5

The practical consequence is that implementing the score directly in the complex domain avoids FFT and reduces triple scoring from eiRde_i \in \mathbb{R}^d6 to eiRde_i \in \mathbb{R}^d7 (Trouillon et al., 2017).

This equivalence is important because it isolates where empirical differences actually arise. The comparison paper shows that discrepancies between original HolE and ComplEx results on FB15K were due to loss functions and training setups, not scoring differences. With one negative per positive, filtered MRR on WN18 was 0.938 for margin loss and 0.941 for logistic negative log-likelihood; on FB15K, the same comparison was 0.541 versus 0.639. Margin yielded better raw MRR but worse filtered metrics on FB15K, suggesting higher overfitting risk (Trouillon et al., 2017).

HolE’s original benchmark results establish its standing among knowledge-graph embedding models. On WN18, HolE achieved filtered MRR 0.938, Hits@1 93.0, Hits@3 94.5, and Hits@10 94.9, compared with RESCAL at MRR 0.890 and TransE at 0.495. On FB15k, HolE achieved filtered MRR 0.524, Hits@1 40.2, Hits@3 61.3, and Hits@10 73.9, compared with RESCAL at MRR 0.354 and TransE at 0.463 (Nickel et al., 2015).

Dataset HolE filtered results Selected comparison
WN18 MRR 0.938; Hits@1 93.0; Hits@3 94.5; Hits@10 94.9 RESCAL MRR 0.890; TransE MRR 0.495
FB15k MRR 0.524; Hits@1 40.2; Hits@3 61.3; Hits@10 73.9 RESCAL MRR 0.354; TransE MRR 0.463

The computational trade-offs are equally explicit. HolE retains fixed-width compositionality with memory complexity eiRde_i \in \mathbb{R}^d8 and FFT-based triple scoring in eiRde_i \in \mathbb{R}^d9. For rpRdr_p \in \mathbb{R}^d0, scoring a triple takes approximately rpRdr_p \in \mathbb{R}^d1, an epoch on WN18 takes approximately rpRdr_p \in \mathbb{R}^d2, and best validation is often reached in 200–500 epochs. On FB15k, example parameter counts were approximately rpRdr_p \in \mathbb{R}^d3M for RESCAL at rpRdr_p \in \mathbb{R}^d4 versus approximately rpRdr_p \in \mathbb{R}^d5M for HolE at rpRdr_p \in \mathbb{R}^d6 (Nickel et al., 2015). ComplEx preserves the same expressive scoring class while shifting the implementation to linear-time complex arithmetic (Trouillon et al., 2017).

A common misconception is therefore that HolE and ComplEx differ fundamentally in what they can represent. The cited comparison argues the opposite: both are equally expressive at the level of the scoring function, while runtime, representation domain, and loss choice determine most practical differences (Trouillon et al., 2017).

4. HKM as a continual-learning substrate for LLMs

A later and substantially different formulation defines HKM as a four-phase pipeline that builds, compresses, integrates, and continuously updates a structured “knowledge substrate” for LLMs without catastrophic forgetting. In this formulation, substrates are unified manifolds of entangled and quantized concept embeddings, represented as a hierarchical graph rpRdr_p \in \mathbb{R}^d7 where rpRdr_p \in \mathbb{R}^d8 are nodes, rpRdr_p \in \mathbb{R}^d9 are probabilistic edges, and a,bRda,b \in \mathbb{R}^d0 are fractal levels. The reported objective is to achieve zero catastrophic forgetting with minimal memory growth by combining probabilistic entanglement, fractal quantization, holographic integration into attention, and dynamic diffraction chipping (Arndt, 3 Sep 2025).

Phase Operation Reported output
Phase A Probabilistic entanglement Entanglement matrix and 2,997 nodes
Phase B Fractal quantization 3× compression, 67% storage savings
Phase C Holographic integration Final loss 2.543, integration 100%
Phase D Dynamic diffraction chipping 0% forgetting, growth ≈1% per update

Phase A computes embeddings a,bRda,b \in \mathbb{R}^d1 from a swarm of small encoders and forms a row-stochastic entanglement matrix through diffusion-like noise injection:

a,bRda,b \in \mathbb{R}^d2

In the reported experiments, the process used preprocessed WikiText snippets and FB15k triples, produced 2,997 nodes, and yielded entanglement entropy empirically a,bRda,b \in \mathbb{R}^d3. The implementation notes specify a GPU-parallel routine with iterations = 35 and swarm_size = 15 (Arndt, 3 Sep 2025).

Phase B reduces dimensionality by PCA to 128 components with 93.3% explained variance and constructs a self-similar, mixed-precision lattice through hierarchical clustering over 5–10 levels. The reported fractal dimension is

a,bRda,b \in \mathbb{R}^d4

with empirical value a,bRda,b \in \mathbb{R}^d5. Operational quantization is performed with torch.quantize_per_tensor_dynamic(..., group_size=128, dtype=torch.qint8), and the reported aggregate outcome is a compression ratio of a,bRda,b \in \mathbb{R}^d6 with 67% storage savings (Arndt, 3 Sep 2025).

Phase C couples the substrate to a fine-tuned Phi-1.5 model through holographic sampling and an attention interference term. A query a,bRda,b \in \mathbb{R}^d7 projects onto manifold nodes via cosine similarity, a,bRda,b \in \mathbb{R}^d8, then zooms along fractal levels to gather multi-scale context. Attention is modified to

a,bRda,b \in \mathbb{R}^d9

Training used Unsloth mixed precision, reached final loss 2.543, and reported “integration measured at 100%,” operationally defined as

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},0

In this usage, “holographic integration at 100%” does not denote an abstract completeness theorem; it denotes that all targeted manifold concepts required by downstream tasks were recoverable and influential during attention (Arndt, 3 Sep 2025).

Phase D introduces continual updates via spectral interference:

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},1

The paper describes this as dynamic diffraction chipping with RL-pruned EWC. The standard forgetting metric

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},2

was reported as (ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},3. Memory growth was reported as approximately 1% per update, with support for more than 1,020 updates before doubling. Reported runtime numbers include GPU Phase 3 at 282.2 s versus CPU approximately 600 s, interpreted as a 53% reduction, together with a 21.2% energy reduction (Arndt, 3 Sep 2025).

The same source also reports hypothetical total-cost and carbon analyses, but those projections are framed as hypothetical rather than as measured training outcomes. The measured experimental setup used a merged WikiText subset and full FB15k to construct a concept graph with 2,997 nodes, and compared against GEM and EWC baselines. A controversy is therefore built into the formulation: the paper presents zero catastrophic forgetting and “infinite improvement” over GEM in forgetting resistance, but this statement is defined relative to the standard forgetting metric and the cited baseline level of approximately 8% (Arndt, 3 Sep 2025).

5. Microscopic holography, area-law capacity, and the burden of memory

A physically motivated interpretation of HKM comes from a bosonic field theory on a (ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},4-dimensional sphere (ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},5 with a momentum-dependent attractive interaction. The field operator is expanded in spherical harmonics,

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},6

with Laplace eigenvalues (ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},7 and level degeneracy scaling as

(ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},8

At critical occupation number of a soft master mode, an entire shell of higher-angular-momentum modes becomes gapless. The number of these gapless modes scales as the area of an (ab)k=i=0d1aib(i+k)modd,(a \star b)_k = \sum_{i=0}^{d-1} a_i b_{(i+k)\bmod d},9, yielding what the paper explicitly describes as an area-law for microstate entropy (Dvali, 2018).

This gapless shell acts as the memory-bearing structure. Pattern states are written as

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.0

where

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.1

The binary memory space therefore has dimension (ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.2 and microstate entropy

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.3

Because the shell is gapless at criticality, the paper argues that an exponentially large number of patterns can be stored within a microscopic energy gap (Dvali, 2018).

The distinctive dynamical feature is “survival by the burden of memory.” When the master occupation deviates from criticality, the formerly gapless shell acquires a gap and stored patterns become energetically costly. The effective leakage amplitude and survival scale are given as

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.4

where (ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.5 is the load of the memory pattern. Heavier loads suppress the amplitude and increase the characteristic survival time, so memory-rich states decay more slowly. The corresponding pattern-energy penalty away from criticality scales as

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.6

In the paper’s language, heavier memories stabilize the state against decay and force information to be off-loaded between successive holographic states rather than escape the system (Dvali, 2018).

The HKM interpretation of this construction is explicit in the supplied material. The boundary-like shell of gapless modes provides the coordinates of the manifold, binary occupations encode knowledge features, and capacity scales as

(ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.7

Controlled off-loading between neighboring shells produces distributed redundancy through scrambling, while external leakage is suppressed by energy mismatch. The paper further suggests a neural instantiation: a network with Laplacian-like spectra and activity-dependent threshold lowering could reproduce shell gaplessness, area-law capacity, and load-dependent robustness (Dvali, 2018).

This physics-based formulation should not be conflated with HolE or with the continual-learning pipeline. It is a microscopic model of holography and memory capacity, later mapped onto HKM terminology. Its significance lies in supplying explicit mechanisms for capacity, robustness, and update through criticality and shell-to-shell transfer.

6. Riemannian semantic mapping, interpolation, and geodesic navigation

A different line of work presents a “knowledge manifold” as a Riemannian geometric space for scientific literature and then distills it into a specification implementable as an HKM. Documents are encoded as character-level TF-IDF vectors with analyzer="char_wb", ngram_range=(4, 7), sublinear_tf=True, norm="l2", max_features=250,000, and min_df=1. In the reported study, (ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.8 documents yielded an actual vocabulary size (ab)k=i=0d1aib(ki)modd.(a * b)_k = \sum_{i=0}^{d-1} a_i b_{(k-i)\bmod d}.9, and cosine distance was defined by

ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),0

Four representative documents are chosen by exhaustive search to maximize summed pairwise cosine distances and fixed to the corners of the unit square; the remaining points are optimized by constrained stress minimization with

ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),1

using ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),2, ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),3, and ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),4 (Okabe et al., 4 Jun 2026).

The “holographic” component is the projection/reconstruction duality. Once the 2D map is fixed, local semantic content at an arbitrary query point ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),5 is reconstructed through Smoothed Particle Hydrodynamics. With ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),6, ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),7, and smoothing length

ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),8

the cubic-spline kernel is

ab=F1(F(a)F(b)),ab=F1(F(a)F(b)),a \star b = \mathcal{F}^{-1}(\overline{\mathcal{F}(a)} \odot \mathcal{F}(b)), \qquad a * b = \mathcal{F}^{-1}(\mathcal{F}(a) \odot \mathcal{F}(b)),9

with normalized weights O(dlogd)O(d\log d)0. The interpolated semantic vector is

O(dlogd)O(d\log d)1

Directional semantic gradients are then computed by central differences with O(dlogd)O(d\log d)2, and the pull-back metric induced by the SPH map is

O(dlogd)O(d\log d)3

Geodesics are obtained by minimizing the discrete Riemannian path energy

O(dlogd)O(d\log d)4

with O(dlogd)O(d\log d)5 segments and L-BFGS-B over the 29 interior points (Okabe et al., 4 Jun 2026).

A second reconstruction operator is Gaussian Process Regression on a 10-dimensional Truncated SVD of the TF-IDF matrix, using a Constant O(dlogd)O(d\log d)6 RBF + White kernel and inputs equal to the fixed 2D coordinates. At a query point, GPR yields a posterior mean, uncertainty estimate, and per-document contribution rates. The paper formalizes the contribution of document O(dlogd)O(d\log d)7 as

O(dlogd)O(d\log d)8

In the reported example with evaluation point O(dlogd)O(d\log d)9, the smoothing length was M=(V,E,L)M=(V,E,L)00, the fitted GPR kernel was M=(V,E,L)M=(V,E,L)01, posterior M=(V,E,L)M=(V,E,L)02, and relative uncertainty M=(V,E,L)M=(V,E,L)03. Directional gradient norms were M=(V,E,L)M=(V,E,L)04 and M=(V,E,L)M=(V,E,L)05, with cosine similarity 0.0296, indicating near-orthogonality at that point (Okabe et al., 4 Jun 2026).

The reported geodesic example ran from M=(V,E,L)M=(V,E,L)06 to M=(V,E,L)M=(V,E,L)07. The adopted initial candidate had amplitude M=(V,E,L)M=(V,E,L)08 and succeeded under the optimizer. Straight-path energy was M=(V,E,L)M=(V,E,L)09, optimized geodesic energy was M=(V,E,L)M=(V,E,L)10, and the energy reduction was M=(V,E,L)M=(V,E,L)11, or approximately 0.2135%. The corresponding Riemannian lengths were 0.33812 for the straight path and 0.33788 for the geodesic, with maximum lateral deviation 0.013586 and anisotropy M=(V,E,L)M=(V,E,L)12 in M=(V,E,L)M=(V,E,L)13 (Okabe et al., 4 Jun 2026).

Within this framework, “virtual knowledge” refers to hypothetical paper abstracts generated from interpolated TF-IDF content at off-document locations in the map. The constraints are strict: describe target, methods, expected results, and significance; do not introduce concepts absent from the TF-IDF vocabulary; do not fabricate data or numeric values; and follow academic abstract style. In HKM terms, the 2D map functions as a holographic screen from which local high-dimensional semantic vectors can be reconstructed and traversed geodesically (Okabe et al., 4 Jun 2026).

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