In S-Theory, the electron’s mass is not treated as a scalar quantity or a point object, but rather as a structured entropy field — a localized distribution of entropy density, centered at the origin and falling off radially. This core field is denoted Score(r) and represents the internal collapsed identity of the electron arising from its rest mass.
3.1. Mathematical Formulation of Score from Electron Mass
(i) The Score Field – Entropy Core of the Electron
We define the core entropy field of the electron, denoted as
Score(r), to represent the structured entropy arising from the electron’s rest mass.
 |
(2) |
Where: Am is the normalization constant for entropy density (not mass), σm is the characteristic width of the Score field.
(ii) From Mass to Entropy: Core Logic
According to S-Theory, mass is structured entropy. Following Einstein:
where
T is an effective entropic temperature — a measure of entropy freedom (low for stable mass). This structured entropy is not spread across all space but localized into a dense core — the
Score field, which stores the “collapsed identity” of the electron. This entropy is highly localized, meaning the field must peak sharply and decay rapidly — consistent with a Gaussian profile. The spatial width
σm is not arbitrary. It is chosen based on the
Compton wavelength λC of the electron:
This defines the natural localization radius of the electron’s core entropy. This corresponds to the natural quantum length scale over which the electron’s wavefunction — or here, entropy field — is confined.
(iii) Normalization of Score Field
We now normalize
Score such that its total integrated entropy corresponds to
Se = kB ln 2, representing
one bit of fundamental entropy — the minimal quantum configurational entropy associated with a spin-½ particle (Ω = 2 microstates). That is,
 |
(5) |
In polar coordinates:
 |
(6) |
This evaluates to:
 |
(7) |
Using:
kBln2 ≈9.57×10−24 J/K
σm=λC=3.86×10−13 m
(iv) Physical Interpretation and justification
This construction yields the Score(r) field as a sharply peaked entropy density centered at the origin and localized at the Compton scale. Its integral gives one bit of structured entropy, meaning: i) Mass becomes a localized entropy configuration, not a constant, ii) The field is sharply confined (~10−13 m), representing the collapsed identity of the electron, iii) Entropy is quantized in discrete bits, even for elementary particles. This approach reinterprets mass as frozen, structured entropy, embedded in space via a measurable field distribution.
This field represents the irreducible structured identity of the electron — the entropy signature associated with its mass. As shown in
Figure 2 (red color field), this field sharply peaks at the center and decays radially. Now we have
a Score that is clearly defined as an entropy field, not a mass density.
σm is set by
Compton wavelength, not arbitrary. The normalization yields a physical entropy unit (e.g., 1 bit, or k
Bln2). This
Score represents a normalized Gaussian entropy density, centered at the origin, which defines the electron’s collapsed mass configuration. The field integrates to
kB ln 2 and is localized at the Compton scale (~10
−13 m), establishing mass as a structured entropy phenomenon in the S-Theory framework.
(v) Why ln 2? The Identity Bit of the Electron
In S-Theory, every stable quantum system must possess a minimal entropy signature anchoring its individuality. For the electron, with spin-½ and Ω = 2 states:
This is not thermal entropy but ontological entropy — a measure of how many
internal configurations a collapsed system can realize. This idea, consistent with quantum information theory, provides a deep bridge between thermodynamics and identity: The
Score field encodes the electron’s “
1 bit of being.”. This assignment does not imply thermal entropy in the conventional sense, but instead defines a minimum ontological entropy associated with the electron’s existence as a distinct, indivisible fermion. In the context of S-Theory, this unit entropy anchors the
Score field, allowing us to treat the electron’s mass as a localized, structured entropy field normalized to a fundamental quantum of identity. This normalization not only aligns with Boltzmann entropy and quantum spin logic but also provides a consistent base for comparing and interpreting the electron’s associated fields — including the spread entropy of charge (
Section 3.2) and the dynamic thermal field during interaction (Section 3.3). In dimensionless units (e.g., setting k
B=1 in natural units), this is:
 |
(9) |
Thus, the electron’s mass is reinterpreted as a field that contains exactly 1 bit of structured entropy — distributed in space such that its Score field integrates to ln2. In practice, some literature (especially in quantum information theory) approximates 1 bit entropy as “2” when expressed as Ω (number of microstates), which gives: S = lnΩ = ln2 ⇒ Ω=2. So, we are not integrating to a value of “2” directly, but rather: to kBln2 in SI units, or 1 bit in information units, or 0.693 in pure math units. We present the mass of the electron as an entropy field (Score), peaked at the center, whose total integral is kBln2— representing one bit of structured entropy associated with the collapsed electron identity.
3.2. Mathematical Formulation of SEM from Charge
The
SEM field represents the distributed electromagnetic entropy associated with the electron’s electric charge. Unlike the
Score field, which is sharply localized due to mass, the
SEM field is spatially broader and reflects the outward entropy radiation of charge. We model it using a radially symmetric Gaussian:
 |
(10) |
Where: Aq is the normalization constant linked to electromagnetic entropy density, σq is the characteristic spread of the field (typically σq > σm).
(i)From Charge to Entropy: The S-Theory Logic
In classical electrodynamics, an electric charge creates a radial Coulomb field that stores
energy. In S-Theory, energy is interpreted as structured entropy:
 |
(11) |
Thus, the Coulomb field around the electron gives rise to a corresponding spread entropy field,
SEM, which encodes the spatial distribution of electromagnetic potential in thermodynamic terms. Rather than normalizing this field to the charge magnitude
∣qe∣, we normalize it to a meaningful entropy quantity. To ensure consistency with the
Score field (
Section 1), we define the total entropy in the
SEM field as:
 |
(12) |
Here, γ is a dimensionless scaling factor reflecting the broader spatial influence of charge compared to mass. Typically, γ>1.
(ii) Choice of Spread Width σq
The spatial spread of the
SEM field is selected to reflect the more diffuse nature of electromagnetic fields. Rather than using the classical electron radius, we define:
 |
(13) |
where
 |
(14) |
λC is the Compton wavelength, and η is a scaling factor. Choosing η=4, we obtain:
σq =4⋅λC ≈ 1.54×10−12 m
This ensures that the SEM field is smoother and more extended than the Score field, in accordance with observed electromagnetic behavior.
(iii) Normalization Constant
Given the Gaussian form of the
SEM field, the entropy normalization gives:
 |
(15) |
For example, with γ=3 and the above value of
σq, we obtain:
 |
(16) |
This yields a broad entropy field that smoothly decays with distance and contributes significantly to the total entropy structure of the electron.
Figure 3.
SEM Entropic EM field distribution of Electron.
Figure 3.
SEM Entropic EM field distribution of Electron.
(iv) Estimation of microstates of SEM: Comparison to Score
In the previous section 2.2, we derived
This corresponds to 1 bit and reflects collapsed identity (a binary quantum choice: spin-up/down, particle/antiparticle, etc.). Now: What Should SEM Represent? The SEM field is: i) spread out, not collapsed ii) derived from electromagnetic field energy iii) not a binary state, but a continuum of influence, so it shouldn’t be just “1 bit” like Score. It should encode more entropy — a distributed informational cloud, not a defined choice.
When we set γ=3, we Are Saying:
 |
(18) |
This is not 3 bits, but:
 |
(19) |
Interpretation: If the Score field represents an electron’s collapsed identity — 1 bit (Ω = 2), then the SEM field represents a more delocalized, entangled field — encoding Ω = 8 possible microstates (i.e., 3 bits of information). What does this tell us? The entropy content of SEM is higher not because it’s more “informative” in a collapse sense, but because it’s spread across more degrees of freedom. While Score = collapsed, bounded, SEM = expanded, radiative, and contains multiple field configurations or “degrees of potential interaction”. So, we might interpret: Score as existence entropy (a single quantum identity), SEM as interaction entropy (the field’s available entangled micro-configurations with space).
(v) What if Gamma Were 5 Instead?
So γ is directly scaling the microstate count of the SEM field:
 |
(20) |
It gives us a semantic handle on field complexity.
Final Summary:
| Field |
Total Entropy S |
Bits |
Microstates Ω |
Meaning |
| Score |
kBln2 |
1 |
2 |
Binary identity (collapse) |
| SEM
|
γ⋅kBln2 |
γ |
2γ
|
Distributed EM interaction entropy |
So, with γ=3, SEM carries 8x more microstate potential than Score.
(vi) Physical Basis of γ — Linked to Spatial Entropy Volume
Entropy depends not only on the amount of energy (charge field), but also on how spread out it is. We define:
 |
(21) |
So: a larger spatial spread (larger
σq) means more possible configurations for the field → higher
ΩEM, higher
γ. A tightly confined field (small
σq) means fewer options → smaller
γ. So
γ is directly tied to the spatial entropy volume:
 |
(22) |
We can think of it as a “configurational volume ratio. What happens to
SEM after the collapse? When a measurement occurs (e.g., detecting charge or interaction):
i) The spread entropy collapses to a localized structure (like a
Score-type).
ii) the system selects one of the
Ω microstates from the
SEM field
ii) So the measured charge corresponds to 1-bit output (Yes: charge detected; No: not detected). So, after the collapse:
 |
(23) |
The rest of SEM’s entropy radiates outward or decoheres, just like a wavefunction collapse in QM.
(vii) Justification of γ = 3 (vs. 10)
Our choice of γ = 3 is: not a guess, but a provisional assignment based on a physical scale:
Since σq/σm=4 and entropy scales with area:
So γ ≈ 3–4 is reasonable based on spatial scaling. If we had chosen: σq=10σm → γ ≈ log(2x100) = 6.6, this would imply 6–7 bits of field complexity — valid only if the electron is embedded in a very high-energy or noisy EM environment. So: γ is not fixed by charge, but by field geometry and available spatial entropy before collapse. So, γ is not arbitrary but tied to the spread radius of the entropy field, charge is constant, but entropy associated with that charge depends on space and configuration freedom, after measurement, only 1 bit remains — the rest is dissipated or encoded elsewhere. So γ captures the pre-collapse entropy potential of the electron’s EM field.
3.4. The Sthermal Field: Entropic Interaction Between Structure and Environment
In the S-Theory framework, the entropy field of a fundamental particle such as the electron is not fully described by mass (Score) and charge (SEM) alone. These fields represent intrinsic, localized (Score) and spatially extended (SEM) components of structured entropy. However, the third and often overlooked dimension is interaction entropy — the distributed and fluctuating entropic field arising from the electron’s coupling to the surrounding environment and vacuum fluctuations. We call this field Sthermal, short for Structured Thermal Entropy.
-
(i)
Origin and Necessity of Sthermal
Whereas Score is derived from the concentrated entropy due to rest mass and SEM from the spread associated with the electromagnetic field, Sthermal arises from external interactions — including temperature-dependent noise, quantum vacuum fluctuations, and photon scattering. It captures the entropy flow into and out of the electron’s system boundary. This makes Sthermal the key dynamic component that determines whether the electron collapses (measurement), radiates (scattering), or remains in a superposed, thermodynamically stable state. Traditionally, quantum mechanics assumes idealized closed systems and primarily models probabilities via the wavefunction. In contrast, S-Theory explicitly recognizes the system’s coupling to its entropic surroundings, leading to a more complete and physically grounded model of the electron as a dynamic structure embedded in a sea of entropy. This aligns closely with open quantum systems and thermofield dynamics, yet goes further by defining a scalar field that measures the residual entropy potential surrounding a quantum object.
-
(ii)
Mathematical Formulation of the Sthermal Field
The
Sthermal field shown in
Figure 4 is constructed as a low-amplitude, wide-spread Gaussian random field added to the entropy profile. Unlike
Score and
SEM, which are symmetric and physically defined by core parameters (mass and charge),
Sthermal is non-symmetric and randomly modulated, representing microscopic stochasticity and interaction history. We define the
Sthermal field over a 2D domain using a low-frequency filtered random noise modulated by a Gaussian envelope:
 |
(25) |
Where: smooth_rand (x, y) is a low-pass filtered 2D random noise (e.g., convolution with a Gaussian kernel), σth is the thermal spread radius, much wider than SEM or Score, A is a small amplitude scaling factor, ensuring Sthermal does not dominate in isolation but strongly modulates during collapse events, the units are normalized entropy density per unit area. This field is then normalized to a maximum of 1 before visualization or summation into the RGB field.
-
(iii)
Physical Interpretation: The Missing Link in QM
The
Sthermal field (
Figure 4) plays several vital roles that are ignored or marginalized in standard QM:
i) entropy exchange: It captures the entropic flow to/from the environment, which is central to the measurement process
ii) collapse sensitivity: the moment a high-energy photon enters the
Sthermal field, recursive amplification of Sfield (RAS) with
SEM can drive the system toward collapse,
iii) entropic equilibration: It defines the thermal envelope in which Score and SEM are modulated — without it, any energy-based picture misses the stochastic interactions needed for life, measurement, or evolution,
iv) time-evolution context: As shown in later sections,
Sthermal governs local entropic time, as used in EPS (Entropy Positioning System [
5]), defining the effective “aging” or dynamic change of field structure over time. Thus, in S-Theory,
Sthermal is not optional.
It is the thermodynamic gradient and stochastic scaffold without which no real system (including electrons, molecules, or brains) can evolve or respond to measurement.
3.5. Combined Entropic Field of an Electron
Figures 5
a–c present a summary of these three entropic subfields individually in color-coded visual form:
Score in red,
SEM in blue, and
Sthermal in green, each emerging from the same radial coordinate space but expressing different spatial scales and intensity gradients.
Figure 5d is the combined entropy field of the electron (RGB Composition). This RGB fusion
total image synthesizes the three entropic components into a single composite field given by equation (26).
 |
(26) |
The red (mass), green (thermal), and blue (charge) channels are superimposed, forming a complete entropy structure of the electron. The bright white center signifies the peak of recursive entropic amplification, where all three fields converge — a region of maximum coherence and minimum uncertainty.
This unified representation provides a visual and thermodynamic map of the electron as a structured entropy field, central to the S-Theory reinterpretation of quantum mechanics. In
Figure 5d, the Sthermal field appears as the green component, forming a diffuse glow enveloping the sharper Score (red-turned white in the combined image
) and
SEM (blue) fields. Its presence transforms the otherwise symmetrical Score–S
EM model into a realistic, fluctuating, field-interactive system, opening the
door to a thermodynamic explanation of uncertainty, wavefunction collapse, and decoherence.
(i) Estimation of microstates of Sthermal: Comparison to Score and SEM
Based on prior modeling, the SEM field is linked to the Score field by a scaling factor γ=3, leading to SEM=3 x Score and an associated increase in microstates from Ωcore=2 to ΩEM=23=8. For the Sthermal field, which has the most significant spatial extent and represents the thermodynamic residue of interaction, we estimate a higher scaling factor α ≈ 5–8 resulting in Sthermal=α⋅Score. This yields a microstate range of Ωthermal = 2α = 32 to 256. Thus, the Sthermal component carries the dominant share of entropy and microstates in the complete Sfield structure. Conceptually, the collapse process compresses this Sthermal cloud and the SEM field toward the Score core, and leaves behind a coherent, spinning entropy structure—giving rise to measurable properties like charge and spin. This expanded entropy perspective, uniquely enabled by S-Theory, restores the missing thermodynamic dimension neglected by traditional quantum mechanics and provides a more complete framework for understanding measurement, decoherence, and particle identity.