scholarly journals The Mirror Reversal Mechanism on Black Hole Collapse and Singularity Eruption in Cosmic Continuum

Author(s):  
Xijia Wang

Abstract In the Big Bang Theory and the Black Hole Theory, the existing laws of physics all fail atthe singularity, and the singularity has become a blind spot in the existing scientific theories. In Cosmiccontinuum, the cosmic system collapse into a Schwarzschild black hole under the action of a stronggravitational field, and the Planck spheres at the center of the black hole continues to collapse into darkmass bodies, forming dark celestial body and singularity. The Schwarzschild radius is the upper limit ofa black hole, and the Planck sphere is the lower limit of a black hole. The singularity is the conversionpoint between the old and new cosmic systems. The singularity erupts the Planck spheres under theaction of a strong gravitational field, and the Planck spheres expands outward to form a new cosmicsystem. The Planck sphere is both the end of the old cosmic system and the starting point of the newcosmic system. The black hole collapse and the singularity eruption are mirror images of each other.The Planck sphere is the front of the mirror, and the singularity is the back of the mirror.

2021 ◽  
Author(s):  
Xijia Wang

Abstract In the Big Bang Theory and the Black Hole Theory, the existing laws of physics all fail atthe singularity, and the singularity has become a blind spot in the existing scientific theories. In Cosmiccontinuum, the cosmic system collapse into a Schwarzschild black hole under the action of a stronggravitational field, and the Planck spheres at the center of the black hole continues to collapse into darkmass bodies, forming dark celestial body and singularity. The Schwarzschild radius is the upper limit ofa black hole, and the Planck sphere is the lower limit of a black hole. The singularity is the conversionpoint between the old and new cosmic systems. The singularity erupts the Planck spheres under theaction of a strong gravitational field, and the Planck spheres expands outward to form a new cosmicsystem. The Planck sphere is both the end of the old cosmic system and the starting point of the newcosmic system. The black hole collapse and the singularity eruption are mirror images of each other.The Planck sphere is the front of the mirror, and the singularity is the back of the mirror.


2021 ◽  
Author(s):  
Xijia Wang

Abstract In Cosmic continuum, the cosmic system collapse into a Schwarzschild black hole under the action of a strong gravitational field, and the Planck spheres at the center of the black hole continues to collapse into dark mass bodies, forming dark celestial body and singularity. The Schwarzschild radius is the upper limit of a black hole, and the Planck sphere is the lower limit of a black hole. The singularity is the conversion point between the old and new cosmic systems. The singularity erupts the Planck spheres under the action of a strong gravitational field, and the Planck spheres expands outward to form a new cosmic system. The Planck sphere is both the end of the old cosmic system and the starting point of the new cosmic system. The black hole collapse and the singularity eruption are mirror images of each other. The Planck sphere is the front of the mirror, and the singularity is the back of the mirror.


2004 ◽  
Vol 01 (03) ◽  
pp. 429-443
Author(s):  
JOEL SMOLLER ◽  
BLAKE TEMPLE

We derive and analyze the equations that extend the results in [20,21] to the case of non-critical expansion k≠0. By an asymptotic argument we show that the equation of state [Formula: see text] plays the same distinguished role in the analysis when k≠0 as it does when k=0: only for this equation of state does the shock emerge from the Big Bang at a finite nonzero speed — the speed of light. We also obtain a simple closed system that extends the case [Formula: see text] considered in [20,21] to the case of a general positive, increasing, convex equation of state p=p(ρ).


2005 ◽  
Vol 20 (26) ◽  
pp. 6039-6049 ◽  
Author(s):  
XIN ZHANG

A toy model based upon the q-deformation description for studying the radiation spectrum of black hole is proposed. The starting point is to make an attempt to consider the space–time noncommutativity in the vicinity of black hole horizon. We use a trick that all the space–time noncommutative effects are ascribed to the modification of the behavior of the radiation field of black hole and a kind of q-deformed degrees of freedom are postulated to mimic the radiation particles that live on the noncommutative space–time, meanwhile the background metric is preserved as usual. We calculate the radiation spectrum of Schwarzschild black hole in this framework. The new distribution deviates from the standard thermal spectrum evidently. The result indicates that some correlation effect will be introduced to the system if the noncommutativity is taken into account. In addition, an infrared cutoff of the spectrum is the prediction of the model.


Author(s):  
F. Melia ◽  
T. M. McClintock

The recent discovery of the ultraluminous quasar SDSS J010013.02+280225.8 at redshift 6.3 has exacerbated the time compression problem implied by the appearance of supermassive black holes only approximately 900 Myr after the big bang, and only approximately 500 Myr beyond the formation of Pop II and III stars. Aside from heralding the onset of cosmic re-ionization, these first and second generation stars could have reasonably produced the approximately 5–20  M ⊙ seeds that eventually grew into z approximately 6–7 quasars. But this process would have taken approximately 900 Myr, a timeline that appears to be at odds with the predictions of Λ CDM without an anomalously high accretion rate, or some exotic creation of approximately 10 5   M ⊙ seeds. There is no evidence of either of these happening in the local Universe. In this paper, we show that a much simpler, more elegant solution to the supermassive black hole anomaly is instead to view this process using the age–redshift relation predicted by the R h = ct Universe, an Friedmann–Robertson–Walker (FRW) cosmology with zero active mass. In this context, cosmic re-ionization lasted from t approximately 883 Myr to approximately 2 Gyr ( 6 ≲ z ≲ 15 ), so approximately 5–20  M ⊙ black hole seeds formed shortly after re-ionization had begun, would have evolved into approximately 10 10   M ⊙ quasars by z approximately 6–7 simply via the standard Eddington-limited accretion rate. The consistency of these observations with the age–redshift relationship predicted by R h = ct supports the existence of dark energy; but not in the form of a cosmological constant.


2015 ◽  
Vol 7 (6) ◽  
pp. 56
Author(s):  
Zifeng Li

<p class="1Body">Analyzes the Big Bang theory, recession of galaxies, Hubble's law, multi-dimensional space, curved space and black hole in modern cosmology and points out that these six theories are all baseless and irrational, contrary to classical science. Promotes the use of plain view of the universe - the materialist view of space–time-mass-energy to study the universe. The observations and understanding of the universe are very limited now. Cosmology should be realistic, not based on irrational models.</p>


Universe ◽  
2018 ◽  
Vol 4 (11) ◽  
pp. 129 ◽  
Author(s):  
Carlo Rovelli ◽  
Francesca Vidotto

Dark matter could be composed by black-hole remnants formed before the big-bang era in a bouncing cosmology. This hypothetical scenario has implications on the issue of the arrow of time: it upsets a common attribution of past low entropy to the state of the geometry and suggests a possible realisation of the perspectival interpretation of past low entropy.


2018 ◽  
Vol 615 ◽  
pp. A113 ◽  
Author(s):  
Fulvio Melia

Aims. The discovery of quasar J1342+0928 (z = 7.54) reinforces the time compression problem associated with the premature formation of structure in Λ cold dark matter (ΛCDM). Adopting the Planck parameters, we see this quasar barely 690 Myr after the big bang, no more than several hundred Myr after the transition from Pop III to Pop II star formation. Yet conventional astrophysics would tell us that a 10 M⊙ seed, created by a Pop II/III supernova, should have taken at least 820 Myr to grow via Eddington-limited accretion. This failure by ΛCDM constitutes one of its most serious challenges, requiring exotic “fixes”, such as anomalously high accretion rates, or the creation of enormously massive (~ 105 M⊙) seeds, neither of which is ever seen in the local Universe, or anywhere else for that matter. Indeed, to emphasize this point, J1342+0928 is seen to be accreting at about the Eddington rate, negating any attempt at explaining its unusually high mass due to such exotic means. In this paper, we aim to demonstrate that the discovery of this quasar instead strongly confirms the cosmological timeline predicted by the Rh = ct Universe. Methods. We assume conventional Eddington-limited accretion and the time versus redshift relation in this model to calculate when a seed needed to start growing as a function of its mass in order to reach the observed mass of J1342+0928 at z = 7.54. Results. Contrary to the tension created in the standard model by the appearance of this massive quasar so early in its history, we find that in the Rh = ct cosmology, a 10 M⊙ seed at z ~ 15 (the start of the Epoch of Reionization at t ~ 878 Myr) would have easily grown into an 8 × 108 M⊙ black hole at z = 7.54 (t ~ 1.65 Gyr) via conventional Eddington-limited accretion.


Author(s):  
Jae-Kwang Hwang

The origins of the stellar mass neutron black holes and supermassive dark matter black holes without the singularities are reported based on the 4-D Euclidean space. The neutron black holes with the mass of mBH = 5 &ndash; 15 msun are made by the 6-quark merged states (N6q) of two neutrons with the mass (m(N6q) = 10 m(n)) of 9.4 GeV/c2 that gives the black hole mass gap of mBH = 3 &ndash; 5 msun. Also, the supermassive black holes with the mass of mSMBH = 106 &ndash; 1011 msun are made by the merged 3-D states (J(B1B2B3)3 particles) of the dark matters. The supermassive black hole at the center of the Milky way galaxy has the mass of mSMBH = 4.1 106 msun that is consistent with mSMBH = 2.08 - 6.23 106 msun calculated from the 3-D states (J(B1B2B3)3 particles) of the dark matters with the mass of m(J) = 1.95 1015 eV/c2. In other words, this supports the existence of the B1, B2 and B3 dark matters with the proposed masses. The first dark matter black hole (primary black hole) was created at the big bang. This first dark matter black hole decayed to the supermassive dark matter black holes through the secondary dark matter black holes that are explained by the merged states of the J(B1B2B3)3 particles. The universe evolution is closely connected to the decaying process of the dark matter black holes since the big bang. The dark matter cloud states are proposed at the intermediate mass black hole range of mIMBH = 102 &ndash; 105 msun. This can explain why the dark matter black holes are not observed at the intermediate mass black hole range of mIMBH = 102 &ndash; 105 msun.


2020 ◽  
Vol 39 (2) ◽  
pp. 183-197 ◽  
Author(s):  
Janelle Pötzsch

This article analyses whether and to what extent the popular TV show The Big Bang Theory conveys anti-intellectual ideas. The starting point of my enquiry is the verbal behaviour of the ‘main nerd’ of this series, Sheldon Cooper, who is noteworthy for his lack of empathy and propriety. I aim to shed light on the kind of inappropriate verbal behaviour Sheldon displays by analysing a speech pattern this character is particularly bad at ‐ ‘white lies’, that is lies made out of consideration for other people’s feelings. By drawing on Immanuel Kant’s thoughts on civility in his Anthropology from a Pragmatic Point of View (1798), I will detail the social implications of white lies and how Sheldon fails in employing them. Doing so will be helpful in establishing why Sheldon’s comments and behaviour appear as outlandish as they do. This in turn provides important insights into the way the televisual text of The Big Bang Theory relates with its audience and the social implications of this connection. I will conclude with the observation that the portrayal of Sheldon Cooper relies heavily on two kinds of stereotypes: anti-intellectual ones and those associated with the ‘nerd’ identity.


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