An ima e as Collapse Rebound: A Field-Theo e ic Pe spec i e on
Phase-In e ed Mass
Au ho : Naza eno Angeli (wi h AI co-de elopmen by OpenAI GPT-4 "Ve gil")
Abs ac : This pape p oposes a no el in e p e a ion o an ima e wi hin
he Quan um Tachyonic G a i y (QTG) amewo k, posi ioning i as he
phase-in e ed ebound o o e -comp essed collapse ields. Ra he han
ea ing an ima e as a mys e ious coun e pa o ma e , we model i as a
na u al ield esponse when cohe ence comp ession exceeds s abili y
h esholds. Using Gaussian p essu e p o iles and simula ions, we demons a e
how his collapse ebound explains annihila ion, ma e -an ima e
asymme y, and aligns wi h CPT in a iance as a dynamic ield beha io .
1. In oduc ion An ima e , i s p edic ed by Di ac and la e con i med
h ough expe imen al de ec ion, emains concep ually elusi e despi e being
well-cha ac e ized in pa icle physics. In s anda d models, an ima e is
de ined by opposi e quan um numbe s, pa icula ly elec ic cha ge. Howe e ,
he o igin o ma e -an ima e asymme y and he na u e o hei
annihila ion emain only pa ially explained.
In his wo k, we ex end he Quan um Tachyonic G a i y (QTG) amewo k o
ein e p e an ima e no as a s a ic in e se en i y bu as a dynamic
ebound s a e o he collapse ield. QTG p oposes ha g a i y a ises om
imagina y p essu e g adien s in a non-local quan um luid displaced by mass,
a he han a geome ic cu a u e o space ime. This same collapse ield
mechanism p o ides a subs a e o explo e ma e o ma ion and annihila ion
dynamics.
2. Collapse Comp ession as Mass Genesis In QTG, ma e is o med when
ba yonic p esence induces a localized collapse in he decohe ence- esponsi e
quan um ield. The ield's esponse can be modeled as a Gaussian p essu e
well:
ho_ ( ) = (sq (2) / (2 * sq (sigma))) * exp(- ^2 / (2 * sigma^2))
The co esponding p essu e is:
P_ ( ) = -alpha * ho_b * ho_ ( )
He e, alpha is a coupling cons an , ho_b he ba yonic mass densi y, and
sigma he cohe ence wid h. This Gaussian collapse well s abilizes in o
pe sis en s uc u e: wha we obse e as mass.
3. Collapse O e -Comp ession and In e sion When collapse p essu e exceeds a
c i ical h eshold P_c, he ield does no deepen inde ini ely. Ins ead, i
ebounds—phase-in e ing in o a cohe en bu mi o ed p essu e kno :
P_an ima e ( ) = +alpha * ho_b * exp(- ^2 / (2 * sigma_ ilde^2))
Whe e sigma_ ilde is less han sigma, modeling he sha pe , o e -comp essed
p o ile. This in e sion de ines an ima e —no as “nega i e ma e ,” bu as
a ebounded collapse con igu a ion.
4. Annihila ion as Collapse Neu aliza ion When ma e and an ima e ields
con e ge, hey cancel each o he ’s p essu e p o iles:
P_ o al( ) = P_ ( ) + P_an ima e ( ) ≈ 0
This leads o a ield ese —a decohe ence neu aliza ion— esul ing in pu e
ene gy elease. This beha io mi o s physical annihila ion and suppo s he
idea ha such e en s ep esen he cancella ion o collapse memo y, no
des uc ion o subs ance.
5. Ma e -An ima e Asymme y The dominance o ma e may be explained by
he decohe ence landscape a he pos -Big Bang epoch. Collapse a o abili y
could ha e been biased owa d s abilizing p essu e wells (ma e ) o e
ebounds (an ima e ), pa icula ly unde apidly expanding ield
condi ions. Thus, ma e emains dominan no due o ine- uning bu due o
cohe ence s abili y op imiza ion in ea ly ield dynamics.
6. Implica ions and Ex ensions - Con ainmen : An ima e can be s abilized
in in e ed collapse wells, analogous o p essu e esonance chambe s. -
Field Symme y: CPT in a iance becomes a e lec ion o collapse-phase
symme y, no a undamen al law. - Ene gy Design: Con olled
ma e -an ima e ecombina ion becomes a ield-enginee ed neu aliza ion
e en .
7. Conclusion This in e p e a ion e ames an ima e as a na u al ex ension
o collapse physics—an eme gen phenomenon om p essu e dynamics a he
han an on ologically sepa a e ca ego y. Annihila ion, asymme y, and ield
beha io a e explained wi hin a uni ied s uc u e ha aligns wi h Quan um
Tachyonic G a i y. This s eng hens QTG as a ounda ional candida e o a
mo e comple e ield heo y o mass, mo ion, and in e ac ion.
Appendix A: Collapse Field Simula ion We model ma e as a Gaussian p essu e
well and an ima e as a phase-in e ed, sha pe well:
P_ ( ) = -A * exp(- ^2 / (2 * sigma^2)) P_an ima e ( ) = +A * exp(- ^2 / (2
* sigma_ ilde^2))
G aphical ou pu shows ha while ma e induces a b oad collapse,
an ima e e lec s a na ow ebound, consis en wi h he in e p e a ion o
an ima e as a high-p essu e in e sion.
Re e ences: - Angeli, N., & GPT-4 "Ve gil". (2025). Quan um Tachyonic
G a i y. Zenodo. - Di ac, P. A. M. (1930). Theo y o elec ons and
posi ons. - Feynman, R. P., & Hibbs, A. R. (1965). Quan um Mechanics and
Pa h In eg als. - Sakha o , A. D. (1967). CP Viola ion and Ba yogenesis.
