Organizations: Department of Computer Science and Engineering, Shahid Beheshti University, Tehran, Iran · School of Computer Science, Institute for Research in Fundamental Sciences (IPM), Tehran, Iran · School of Physics, Engineering and Computer Science, University of Hertfordshire, Hatfield, UK · Department of Computer and Data Sciences, Faculty of Mathematical Sciences, Shahid Beheshti University, Tehran, Iran · Department of Cognitive Modeling, Institute for Cognitive and Brain Sciences, Shahid Beheshti University, Tehran, Iran · International Business University, Toronto, ON, Canada
Kolmogorov-Arnold Networks (KANs) replace fixed scalar weights by learnable univariate maps, yet most spectral KANs still rely on Chebyshev polynomials that live on a bounded interval and therefore require a saturating squashing of the pre-activation. We introduce the Fractional Hermite Kolmogorov-Arnold Network (FHKAN), a neural architecture that equips KANs with an adaptive, trainable fractional-order generalized Hermite basis. With a nonnegative shape parameter, the underlying generalized Hermite functions are orthonormal on the entire real line and uniformly bounded under a Gaussian envelope, so they act directly on unbounded pre-activations without any saturating map. We derive closed-form derivatives of the generalized, fractional, and scaled basis away from the origin and determine its order of differentiability at the origin, where the fractional power map creates a singular point. On synthetic regression, FHKAN attains the lowest test error at every network depth among nine fixed activations and the spline-based KAN. On image classification, image denoising, and sentiment analysis, the best-performing fractional Hermite block yields the highest accuracy or reconstruction quality. On physics-informed problems, FHKAN reaches mean absolute errors of order 10^-6 to 10^-5 on the Lane-Emden equation, residuals of order 10^-4 on the Burgers equation, and absolute errors below 10^-4 on a fractional delay differential equation.
Figures & tables
Basis family of the KAN variant
Natural domain
References
B-splines (original KAN)
bounded, local
[ 14 , 15 , 16 , 20 ]
Wavelets
bounded/local
[ 22 ]
Fourier bases
periodic
[ 23 ]
Radial basis functions
local
[ 24 ]
Temporal/recurrent bases
sequential
[ 25 , 19 ]
Smooth structural bases
bounded
[ 26 ]
Table 1: Summary of Kolmogorov–Arnold Network variants grouped by the univariate basis family used as edge functions, the natural domain on which each family is defined, and the corresponding references. Only the proposed fractional generalized Hermite basis operates natively on the entire real line.
Symbol
Type
Meaning
ζ,ζp
vector, scalar
input of the network and its p -th component
χ,χ^
network map
target function and the map realized by the network
ψ
network map
task-dependent output map of a multi-layer perceptron (distinct from the Hermite functions ψn(μ) )
Θ(i),b(i)
parameters
weight matrix and bias of layer i
θp,q
parameter
expansion coefficient of order q on input p
σ
univariate
fixed scalar activation, or the logistic sigmoid
Table 2: Summary of the notation. Lower-case symbols denote univariate functions and upper-case symbols denote network-level maps.
Figure 2: Fractional Hermite functions defined in ( 13 ). They are bounded, decay at infinity, and stay defined on the whole real line for every admissible γ , so they can be evaluated directly on the unbounded pre-activation of a linear layer.
Figure 3: The fractional Hermite neural block defined in ( 14 ). A pre-activation ζ is rescaled by λ^ , passed through the odd fractional map of order γ^ , and expanded on the generalized Hermite function of order q and shape μ^ . The three parameters λ , γ , and μ (dashed) are trained end-to-end through their smooth reparametrizations.
Figure 4: The two FHKAN topologies used in the experiments.
Figure 5: Synthetic regression study. FHKAN is more accurate than standard activations and the vanilla KAN, its trainable parameters converge quickly, and its run time stays well below that of the spline-based KAN.
Act. func.
Number of hidden layers
1
3
5
7
9
Softplus
0.461 ± 0.046
0.448 ± 0.031
0.448 ± 0.017
0.418 ± 0.078
0.358 ± 0.107
SiLU
0.518 ± 0.125
0.388 ± 0.156
0.363 ± 0.344
0.162 ± 0.128
0.272 ± 0.380
SELU
0.677 ± 0.087
0.384 ± 0.151
0.147 ± 0.058
0.158 ± 0.075
0.127 ± 0.069
Leaky ReLU
0.489 ± 0.086
0.316 ± 0.140
0.214 ± 0.103
0.235 ± 0.067
0.189 ± 0.093
GELU
0.542 ± 0.134
0.165 ± 0.066
0.322 ± 0.616
0.075 ± 0.041
0.252 ± 0.618
Table 3: Test MAE across increasing depth for the synthetic regression experiment.
Act. func.
MAE
MSE
RMSE
Loss
ReLU
0.520±0.101
0.3425±0.1291
0.575±0.106
0.4035±0.1113
Tanh
0.875±0.012
0.9343±0.0396
0.966±0.021
0.9820±0.0471
KAN
0.379±0.051
0.0437±0.0492
0.433±0.049
0.1731±0.0387
FHKAN(5)
0.074±0.026
0.0127±0.0078
0.107±0.036
0.0038±0.0024
FHKAN(6)
0.058±0.017
0.0086±0.0059
0.087±0.032
0.0025±0.0016
Table 4: Single-layer regression metrics for the synthetic regression experiment.
Figure 6: Convolutional architecture used for MNIST classification. The activation blocks are replaced by sigmoid, tanh, ReLU, or an fHNB.
Act. func.
Loss
Accuracy (%)
Sigmoid
0.0611±0.0031
98.092±0.0814
Tanh
0.0322±0.0018
98.904±0.0572
ReLU
0.0256±0.0013
99.140±0.0386
fHNB(2)
0.0249±0.0016
99.156±0.0471
fHNB(3)
0.0227±0.0018
99.211±0.0762
fHNB(4)
0.0209±0.0012
99.272±0.0508
Table 5: Loss and accuracy of a convolutional classifier on MNIST for different activation functions.
Figure 7: Training curves on MNIST. The FHKAN curve reaches a lower validation loss and a higher validation accuracy than the sigmoid, tanh, and ReLU networks from the first epoch onward.
Figure 8: Convolutional autoencoder used for Fashion-MNIST denoising. The activation is selected among sigmoid, tanh, ReLU, or an fHNB.
Act. func.
Pre-train
Denoising
MSE
PSNR
SSIM
MSE
PSNR
SSIM
Sigmoid
0.018± 0.0024
18.03± 0.64
0.579± 0.038
0.018± 0.0016
17.81± 0.29
0.564± 0.016
Tanh
0.017± 0.0017
18.08± 0.48
0.583± 0.029
0.018± 0.0013
17.83± 0.32
0.562± 0.023
ReLU
0.017± 0.0014
18.12± 0.26
0.577± 0.021
0.019± 0.0018
17.54± 0.21
0.537± 0.011
fHNB(5)
0.013± 0.0011
19.24± 0.27
0.649± 0.012
0.017± 0.0008
18.17± 0.25
0.586± 0.012
fHNB(6)
0.012± 0.0009
19.31± 0.28
0.653± 0.016
0.016± 0.0012
18.24± 0.22
0.589± 0.010
Table 6: Fashion-MNIST denoising quality. Higher PSNR and SSIM and lower MSE are better; the best mean in each column is shown in bold.
Figure 9: One-dimensional convolutional network used for IMDB sentiment analysis. The activation is sigmoid, tanh, ReLU, or an fHNB.
Act. func.
Loss
Accuracy
Precision
Recall
F1 -score
ROC-AUC
Sigmoid
0.364± 0.028
84.884± 0.412
84.473± 1.274
85.480± 1.186
84.974± 0.871
92.303± 0.361
Tanh
0.442± 0.047
84.672± 0.693
84.834± 2.318
84.440± 2.147
84.636± 1.579
92.264± 0.448
ReLU
0.416± 0.051
86.320± 0.974
86.554± 1.836
86.000± 1.092
86.276± 1.065
93.366± 0.337
fHNB(1)
0.407± 0.058
86.988± 0.982
87.140± 2.541
86.784± 2.463
86.961± 1.769
94.475± 0.429
fHNB(2)
0.379± 0.033
87.416± 0.524
87.154± 1.128
87.768± 0.947
87.460± 0.737
94.681± 0.392
fHNB(3)
0.418± 0.041
87.156± 0.638
87.800± 1.492
86.304± 1.173
87.046± 0.945
94.495± 0.351
Table 7: IMDB sentiment-classification metrics. The best mean in each column is shown in bold.
Method family
References
Meshless methods
[ 82 , 83 , 84 ]
Finite difference and multistep methods
[ 85 , 86 ]
Variational and perturbation iteration methods
[ 87 , 88 , 89 ]
Spectral and pseudo-spectral methods
[ 90 , 91 , 67 ]
Analytical and semi-analytical methods
[ 92 , 93 , 94 ]
Reproducing kernel Hilbert space methods
[ 95 , 96 , 97 ]
Table 8: Summary of the principal families of methods proposed in the literature for solving Lane–Emden type equations, compiled in the spirit of the comparative tables of [ 81 ] .
Figure 10: Mapped Hermite–Gauss collocation nodes (roots of HN+1 pushed through ( 11 )) and a uniform grid on a truncated interval [0,16] . Under ( 11 ) the origin is the image of ω=−∞ . The nodes cluster near ζ=0 , where the coefficient 2/ζ is singular.
Figure 11: Lane–Emden profiles for m=0,…,5 obtained with the parallel FHKAN (markers) against the reference solutions (solid lines). The domain is the semi-infinite interval [0,+∞) . For m=2,3,4 the reference is a high-order numerical solution.
m
Reference first root
FHKAN
Absolute error
MAE
MSE
Loss
0
2.44948974 (exact)
2.44949712±1.8×10−6
(7.37±1.8)×10−6
(2.14±0.38)×10−6
(6.81±2.30)×10−12
(4.1±0.8)×10−8
1
3.14159265 (exact)
3.14159083±4.7×10−7
(1.82±0.47)×10−6
(1.47±0.29)×10−6
(3.22±0.93)×10−12
(3.6±0.7)×10−8
2
4.35287460 (Horedt)
4.35287902±1.1×10−6
(4.42±1.1)×10−6
(3.85±0.81)×10−6
(2.41±0.86)×10−11
(5.8±1.2)×10−8
3
6.89684862 (Horedt)
6.89684723±3.6×10−7
(1.39±0.36)×10−6
(2.26±0.47)×10−6
(8.05±3.01)×10−12
(6.2±1.4)×10−8
4
14.9715463 (Horedt)
14.9716277±1.9×10−5
(8.14±1.9)×10−5
(4.12±0.96)×10−5
(2.73±1.17)×10−9
(2.1±0.4)×10−7
5
∞ (exact)
no finite root
—
(6.51±1.27)×10−6
(6.02±2.19)×10−11
(7.4±1.5)×10−8
Table 9: First positive root of the Lane–Emden solution on [0,+∞) , together with the pointwise mean absolute error, the mean squared error, and the collocation residual loss. For m=0,1 the reference is exact; for m=2,3,4 it is Horedt’s numerical table [ 80 ] ; for m=5 there is no finite root. MAE and MSE are computed against the exact solution for m=0,1,5 and against the Horedt/RK reference for m=2,3,4 . The loss column is the collocation residual.
Figure 12: Burgers equation solved with the parallel FHKAN for (m0,m1,m2)=(1,0.01,0.1) (top) and (0.1,10−4,0.5) (bottom). The computational domain is (ζ,τ)∈[0,1]×[0,1] ; collocation uses a 100×100 tensor product of mapped Hermite–Gauss nodes.
Figure 13: Fractional delay differential equation solved with the parallel FHKAN: prediction (left), absolute error against the exact solution (center), and residual loss during training (right).
Figure 14: Parameter efficiency on the synthetic regression target, scored against the noiseless function. Markers compare a spline KAN, a Chebyshev KAN, and FHKAN(5) at hidden widths h=5 and h=8 . The marker color, read on the right-hand color bar, gives the mean training time. The Pareto frontier collects the models for which no other model is both more accurate and smaller.
Axiom Research Group · Dept. of Applied Mathematics and Computational Science, NM-AIST, Arusha, Tanzania · AIMS Research and Innovation Centre, Kigali, Rwanda