Gravitational Well - Revision history

MMONTAGEe at 14:40, July 2, 2025

2025-07-02T14:40:26Z

← Older revision		Revision as of 14:40, July 2, 2025
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	This graviton-rich cloud exerts a powerful, yet non-uniform, gravitational attraction toward the core. Unlike a traditional singularity, which is classically considered a point of infinite density and zero volume, the '''Graviton Foam Field''' behaves as a dynamic quantum structure—chaotic, indeterminate, and inherently uncertain in spatial resolution.		This graviton-rich cloud exerts a powerful, yet non-uniform, gravitational attraction toward the core. Unlike a traditional singularity, which is classically considered a point of infinite density and zero volume, the '''Graviton Foam Field''' behaves as a dynamic quantum structure—chaotic, indeterminate, and inherently uncertain in spatial resolution.
			[[File:SuperGravity Gravitational Well.jpg\|left\|thumb\|498x498px\|@ScienceClic]]

	The larger the Gravitational Well, the weaker the gravitational intensity of this cloud becomes. As the system scales, the probabilistic nature of graviton distribution increases, leading to theoretical gravitational dilution. This implies that in the most massive Wells, such as supermassive gravitational wells, there may exist marginal zones within the Baltzov Ring where gravity weakens just enough to permit transient survival.		The larger the Gravitational Well, the weaker the gravitational intensity of this cloud becomes. As the system scales, the probabilistic nature of graviton distribution increases, leading to theoretical gravitational dilution. This implies that in the most massive Wells, such as supermassive gravitational wells, there may exist marginal zones within the Baltzov Ring where gravity weakens just enough to permit transient survival.

MMONTAGEe at 12:58, June 16, 2025

2025-06-16T12:58:37Z

← Older revision		Revision as of 12:58, June 16, 2025
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	<math mode="display" fleqn>\vec{Գ}\underset{\vec{}}{Գ}(r,\theta)		<math mode="display" fleqn>\vec{Գ}\underset{\vec{}}{Գ}(r,\theta)
	= \dot{Գ}\underset{\cdot}{G}(r)		= \dot{Գ}\underset{\cdot}{Գ}(r)
	\;-\;\frac{2 G\, a\, \sin^2\!\theta}{c^3\,r^2}\,		\;-\;\frac{2 G\, a\, \sin^2\!\theta}{c^3\,r^2}\,
	\Bigl(\,L_c + \!\int_0^r\! \ell(r')\,dr'\Bigr)		\Bigl(\,L_c + \!\int_0^r\! \ell(r')\,dr'\Bigr)

MMONTAGEe at 09:17, June 14, 2025

2025-06-14T09:17:58Z

← Older revision		Revision as of 09:17, June 14, 2025
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	{{DSTheme}}{{DSLogo}} {{DSTimeline24to26}}{{DiegeticDS}}		{{DSTheme}}{{DSLogo}} {{DSTimeline24to26}}{{DiegeticDS}}
	----		----
			<blockquote>"The horizon of the black hole is no longer a place in space, but a moment in our past. And the centre of the black hole is no longer a point, but an event in our future... a destiny we cannot avoid"</blockquote>
	{{TerminalLook		{{TerminalLook

MMONTAGEe at 21:30, June 11, 2025

2025-06-11T21:30:28Z

← Older revision		Revision as of 21:30, June 11, 2025
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	This "sticking" effect reveals a profound truth: the degrees of freedom responsible for encoding information do not reside deep inside the gravitational well, but on or just outside the horizon itself. This aligns with the Holographic Principle, which posits that all information within a volume of space can be described by degrees of freedom on the boundary of that space.		This "sticking" effect reveals a profound truth: the degrees of freedom responsible for encoding information do not reside deep inside the gravitational well, but on or just outside the horizon itself. This aligns with the Holographic Principle, which posits that all information within a volume of space can be described by degrees of freedom on the boundary of that space.

	Through the AdS/CFT correspondence, a 5D supersymmetric gravitational well (such as a charged, rotating BPS ~~black~~ ~~hole~~ in <math>AdS_5</math>) corresponds to a thermal state in a 4D conformal field theory (CFT). In this dual picture:		Through the AdS/CFT correspondence, a 5D supersymmetric gravitational well (such as a charged, rotating BPS gravitational well in <math>AdS_5</math>) corresponds to a thermal state in a 4D conformal field theory (CFT). In this dual picture:

	*The entropy of the gravitational well arises from counting quantum states in the boundary field theory.		*The entropy of the gravitational well arises from counting quantum states in the boundary field theory.

MMONTAGEe at 10:30, June 11, 2025

2025-06-11T10:30:46Z

← Older revision		Revision as of 10:30, June 11, 2025
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	{\| class="article-tabled"		{\| class="article-tabled"
	\|		\|
	!<center>[[File:~~High~~ ~~Charge,~~ ~~High~~ ~~Spin Gravitational Well~~.~~png~~\|450px\|center]]</center>		!<center>[[File:Kerr-Reissner-Nordstrom Extreme Case GW.mp4\|450px\|center]]</center>
	!<center>[[File:Young Gravitational Well.png\|450px\|center]]</center>		!<center>[[File:Young Gravitational Well.png\|450px\|center]]</center>
	\|-		\|-
	\|		\|
	!<center>~~High Charge and High~~ Kerr ~~Spin~~ Gravitational Well, with distorted event horizon and ergosphere</center>		!<center>Extreme Kerr-Reissner-Nordström (Newman) Gravitational Well, with distorted event horizon and ergosphere</center>
	!<center>Young Gravitational Well</center>		!<center>Young Gravitational Well</center>
	\|}		\|}

MMONTAGEe at 17:22, June 10, 2025

2025-06-10T17:22:08Z

← Older revision		Revision as of 17:22, June 10, 2025
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	=Entropy of SuperSymmetric Gravitational Well=		=Entropy of SuperSymmetric Gravitational Well=
	With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB strings become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.		With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB strings become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, <math>NS5</math>-branes, and F-strings.

	These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of [[The Bridges]], the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.		These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of [[The Bridges]], the interdimensional pathways in higher-dimensional space. An <math>NS5</math>-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.

	In an exotic and stable configuration known as a BPS Gravitational Well, the 5D geometry forms a bound state of multiple branes and strings. This bound state preserves a fraction of supersymmetry and minimizes energy, leading to stability even in extreme gravitational conditions. The entropy of such a gravitational well corresponds to the total number of distinct microstates—different internal configurations of branes and strings—that share the same macroscopic quantum numbers (mass, angular momentum, charge, etc.).		In an exotic and stable configuration known as a BPS Gravitational Well, the 5D geometry forms a bound state of multiple branes and strings. This bound state preserves a fraction of supersymmetry and minimizes energy, leading to stability even in extreme gravitational conditions. The entropy of such a gravitational well corresponds to the total number of distinct microstates—different internal configurations of branes and strings—that share the same macroscopic quantum numbers (mass, angular momentum, charge, etc.).

MMONTAGEe at 13:16, June 10, 2025

2025-06-10T13:16:35Z

← Older revision		Revision as of 13:16, June 10, 2025
Line 150:		Line 150:

	=Entropy of SuperSymmetric Gravitational Well=		=Entropy of SuperSymmetric Gravitational Well=
	With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB ~~string theories~~ become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.		With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB strings become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.

	These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of [[The Bridges]], the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.		These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of [[The Bridges]], the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.
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	*The entropy of the gravitational well arises from counting quantum states in the boundary field theory.		*The entropy of the gravitational well arises from counting quantum states in the boundary field theory.
	*These quantum states map precisely to the string/brane configurations in the hyperplane.		*These quantum states map precisely to the string/brane configurations in the hyperplane.
	*The match between CFT state-counting and string~~-theoretic~~ entropy confirms the "strings-at-the-boundary" view.		*The match between CFT state-counting and string entropy confirms the "strings-at-the-boundary" view.

	Thus, all information about matter falling into a gravitational well is encoded at or near the horizon, never truly lost or buried in the core. Instead, the horizon behaves as a quantum memory surface, where the degrees of freedom are not just gravitational—but string~~-theoretic~~ in nature.		Thus, all information about matter falling into a gravitational well is encoded at or near the horizon, never truly lost or buried in the core. Instead, the horizon behaves as a quantum memory surface, where the degrees of freedom are not just gravitational—but ''string'' in nature.

	=GW Burst Event / AdS Weather=		=GW Burst Event / AdS Weather=

MMONTAGEe: first correlation to bridge and wells

2025-06-10T13:12:58Z

first correlation to bridge and wells

← Older revision		Revision as of 13:12, June 10, 2025
Line 152:		Line 152:
	With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB string theories become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.		With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB string theories become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.

	These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of The Bridges, the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.		These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of [[The Bridges]], the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.

	In an exotic and stable configuration known as a BPS Gravitational Well, the 5D geometry forms a bound state of multiple branes and strings. This bound state preserves a fraction of supersymmetry and minimizes energy, leading to stability even in extreme gravitational conditions. The entropy of such a gravitational well corresponds to the total number of distinct microstates—different internal configurations of branes and strings—that share the same macroscopic quantum numbers (mass, angular momentum, charge, etc.).		In an exotic and stable configuration known as a BPS Gravitational Well, the 5D geometry forms a bound state of multiple branes and strings. This bound state preserves a fraction of supersymmetry and minimizes energy, leading to stability even in extreme gravitational conditions. The entropy of such a gravitational well corresponds to the total number of distinct microstates—different internal configurations of branes and strings—that share the same macroscopic quantum numbers (mass, angular momentum, charge, etc.).

MMONTAGEe at 10:25, June 10, 2025

2025-06-10T10:25:06Z

← Older revision		Revision as of 10:25, June 10, 2025
Line 148:		Line 148:

	This process leads to a net loss of curvature-energy in the Gravitational Well. However, the system remains in quasi-equilibrium. The interior graviton foam is continuously replenished by incoming matter or through high-frequency dual-graviton interactions, sustaining the energy density and maintaining the probabilistic structure of the Well’s interior. Thus, the Gravitational Well is not a static prison of spacetime, but a dynamic quantum system where energy, curvature, and information continuously flux across the boundary of existence itself.		This process leads to a net loss of curvature-energy in the Gravitational Well. However, the system remains in quasi-equilibrium. The interior graviton foam is continuously replenished by incoming matter or through high-frequency dual-graviton interactions, sustaining the energy density and maintaining the probabilistic structure of the Well’s interior. Thus, the Gravitational Well is not a static prison of spacetime, but a dynamic quantum system where energy, curvature, and information continuously flux across the boundary of existence itself.

			=Entropy of SuperSymmetric Gravitational Well=
			With the emergence of Mark Cooper’s unified framework for M-Cosmology, renewed attention has been given to the entropy of Gravitational Wells, especially within the context of higher-dimensional supergravity. When principles of Supersymmetry (SUSY) are combined with General Relativity, particularly in relativistic cosmological regimes where Type IIA/IIB string theories become relevant, supersymmetric gravitational wells can be constructed from intricate configurations of D-branes, NS5-branes, and F-strings.

			These structures give rise to five-dimensional gravitational wells, objects deeply associated with the essence of The Bridges, the interdimensional pathways in higher-dimensional space. An NS5-brane, in this context, is a five-dimensional hypersurface (with a 6D worldvolume including time), capable of hosting complex brane-string dynamics, and gives rise to either Type IIA or Type IIB string behavior depending on the specific dualities involved.

			In an exotic and stable configuration known as a BPS Gravitational Well, the 5D geometry forms a bound state of multiple branes and strings. This bound state preserves a fraction of supersymmetry and minimizes energy, leading to stability even in extreme gravitational conditions. The entropy of such a gravitational well corresponds to the total number of distinct microstates—different internal configurations of branes and strings—that share the same macroscopic quantum numbers (mass, angular momentum, charge, etc.).

			Open strings end on D-branes that wrap around or near the event horizon. These strings represent quantum excitations of the horizon-bound degrees of freedom. From the perspective of an external observer, when a particle falls toward the gravitational well, it never truly crosses the horizon. Due to infinite redshift near the event horizon, it appears to "stick" at the boundary.

			This "sticking" effect reveals a profound truth: the degrees of freedom responsible for encoding information do not reside deep inside the gravitational well, but on or just outside the horizon itself. This aligns with the Holographic Principle, which posits that all information within a volume of space can be described by degrees of freedom on the boundary of that space.

			Through the AdS/CFT correspondence, a 5D supersymmetric gravitational well (such as a charged, rotating BPS black hole in <math>AdS_5</math>) corresponds to a thermal state in a 4D conformal field theory (CFT). In this dual picture:

			*The entropy of the gravitational well arises from counting quantum states in the boundary field theory.
			*These quantum states map precisely to the string/brane configurations in the hyperplane.
			*The match between CFT state-counting and string-theoretic entropy confirms the "strings-at-the-boundary" view.

			Thus, all information about matter falling into a gravitational well is encoded at or near the horizon, never truly lost or buried in the core. Instead, the horizon behaves as a quantum memory surface, where the degrees of freedom are not just gravitational—but string-theoretic in nature.

	=GW Burst Event / AdS Weather=		=GW Burst Event / AdS Weather=

MMONTAGEe at 08:41, June 10, 2025

2025-06-10T08:41:49Z

@@ Line 24: / Line 24: @@
 =Overview=
 [[File:GW Bridge DS.png|thumb|Cartographic Symbol Associated with Gravitational Wells]]
-'''Condensed Gravitational Space and Time Well, (CGSTW),''' more commonly known as the '''Gravitational Well,''' is a region in space characterized by an extraordinarily dense concentration of an exotic supersymmetric partner of the Graviton particle, called '''Gravitinos.''' These regions arise when a massive star reaches the end of its life, progressing beyond the Neutron Star phase. The extreme pressure within the collapsing core of a Neutron Star forces neutrons, composed of quarks, to crush into one another, forming Gravitinos. This exotic matter is theorized to exist only under the immense pressures and gravitational stresses found in such extreme environments.
+'''Condensed Space and Time Well, (CSTW),''' more commonly known as the '''Gravitational Well,''' is a region in space characterized by an extraordinarily dense concentration of an exotic supersymmetric partner of the Graviton particle, called '''Gravitinos.''' These regions arise when a massive star reaches the end of its life, progressing beyond the Neutron Star phase. The extreme pressure within the collapsing core of a Neutron Star forces neutrons, composed of quarks, to crush into one another, forming Gravitinos. This exotic matter is theorized to exist only under the immense pressures and gravitational stresses found in such extreme environments.
 The '''Graviton Foam Field''', or the '''Baltzov Ring,''' named in honor of '''Alder Baltzov (Альдер Бальцев)''' is a diffuse, cloud-like region that surrounds the core of a Gravitational Well. It arises from the excitation of the Graviton Quantum Field, manifesting as quantum fluctuations in the spacetime metric tensor <math>\large g_{\mu \nu}</math>. Within the core, immense compressive forces generate nanometric fractures, microscopic cracks in the fabric of core matter through which high-energy streams of gravitons escape. These escaping gravitons further excite the surrounding field, giving rise to a self-reinforcing probabilistic cloud of quantum gravitational particles interior.
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 |}
 </div>
 =Domains=
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 One prevailing hypothesis suggests that this cocoon may be the remnants of the progenitor star’s outer layers, gently surrendered during collapse. In the absence of violent rotational forces, the matter could have remained gravitationally bound, forming a quiescent shell. Over time, thermal friction and gravitational compression may have caused the cocoon to heat and emit radiation, mimicking certain properties of traditional accretion but governed by a radically different mechanism.
 =C Speed Violation of the model's Core=