How thick is a black hole event horizon?

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Discussion Overview

The discussion revolves around the concept of the event horizon of a Schwarzschild black hole, specifically addressing its "thickness" and the implications of this characteristic in the context of general relativity and quantum mechanics. Participants explore theoretical aspects, entropy, and the nature of information related to black holes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions the thickness of the event horizon, suggesting it may relate to Planck length or area, and discusses the behavior of photons near the horizon.
  • Another participant states that, according to classical general relativity, the event horizon is considered a surface that is infinitely thin.
  • Some participants mention the relationship between black hole entropy and the surface area of the horizon, noting that this is a general feature of horizons, not just black holes.
  • There is a discussion about the concept of a "stretched horizon," which is posited to be a layer above the event horizon, potentially around one Planck length thick, and its implications for particle absorption and Hawking radiation.
  • Participants express uncertainty about the specific thickness of the horizon and its implications for quantum black hole analysis, with references to various theoretical frameworks.
  • One participant notes the complexity of distinguishing between different types of horizons, such as absolute and apparent horizons, and their respective characteristics.
  • There are mentions of cosmic event horizons and their relationship to information retention, particularly in the context of dark energy and cosmic expansion.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the thickness of the event horizon or the implications of this characteristic. Multiple competing views and interpretations remain, particularly regarding the nature of horizons and their physical properties.

Contextual Notes

Participants highlight the need for clarity on definitions and the complexity of the mathematical constructs involved in black hole physics. There are unresolved questions regarding the dependence on specific theoretical frameworks and the implications of horizon characteristics.

europa1
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hi, I am not a physicist so sorry if this is a stupid question, its just curiosity.

how thick is the light like event horizon of a schwarzschild black hole,
for instance, what the closest distance scale that an infalling photon and an escaping photon be, and whatI is "inbetween"? I've heard that when observed from outside you would never see the photon reach the EH,it just slows and becomes flattened against it,but from the photons point of view nothing out of the ordinary happens,it just crosses the horizon into what seems like normal flat space time,though the maths shows something dramatic has occurred when you pass r = 2MG. is this "thickness" Planck length or area or something else?
 
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As far as classical GR is concerned, it is a surface. That is, infinitely thin.
 
to
espen180thanks, i saw a couple of lectures about the entropy of such a BH and that the maximum entropy of any region of space is its,slightly smaller i think, bounded area in Planck units and not volume and was just in wonder at how much goes on there.
 
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a BH and that the maximum entropy of any region of space is its,slightly smaller i think, bounded area in Planck units and not volume and was just in wonder at how much goes on there.

A somewhat puzzling aspect of black holes is that their information content is proportional to the surface area of the horizon rather than the volume of the interior...this is a general feature of such horizons, not just black hole horizons...a related feature is that everytime a larger horizon is envisioned, it too encapsulates all the interior information...in other words every time you look at a larger horizon all the information is THERE...so exactly where is the information content is located is somewhat puzzling...is observer dependent.

While the entropy of a black hole is large, it is not maximu...it it were the black hole would be stable and in fact they slowly decay..via Hawking radiation...

Seems we have much to learn about horizons, information and entropy.
 
@Naty1

many thanks,i have a lot to learn before i can think intelligently about theoretical physics.
 
Just for added encouragement, cosmology has reached a stage where advanced knowledge of particle physics and quantum mechanics is extremely valuable - not to mention the Phd level skills you need in mathematics.
 
@Chronos
thanks,you are right and hopefully during my lifetime i may gain some understanding,nevertheless i will always keep a towel handy.
 
europa1 said:
...is this "thickness" Planck length ...?

I've repeatedly seen that kind of "thickness" or horizon fuzziness postulated and used in the analysis of BH. I'm sorry but I cannot recall if the tolerance used is always Planck length or some multiple of it. This is just my unreliable impression but what I recall is that people analyzing the effect of dropping something into a BH consider that the particle (or whatever) is morally part of the BH as soon as it comes within this designated "thickness" of the event horizon. My impression is that this plays a significant role in some of the analysis.

I may not be able to find a link for you which illustrates this. But someone else may find it easy to provide one.
EDIT: Europa, I went and quickly looked at three recent LQG black hole papers where (among other things) they were analyzing what happens when you drop a test particle into a BH and it gets absorbed and the horizon area increases and settles at a new level etc. In no case could I find this "finite thickness" invoked. But I remember seeing it in several papers some time back, not necessarily LQG papers, possibly in some other framework. I strongly suspect that your intuition is correct, quantum BH analysis does require some Planck scale indeterminacy of radius and/or horizon area. But I can't help you with a link to a paper where that is made explicit. Hopefully someone else will be able to.
 
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Marcus:
what I recall is that people analyzing the effect of dropping something into a BH consider that the particle (or whatever) is morally part of the BH as soon as it comes within this designated "thickness" of the event horizon.

These mathematical constructs are not easy to unravel via some ascribed physicality and would seem to require you to specify the type of horizon one is discussing: absolute, relative or stretched.

The stretched horizon does not seem to be frequently discussed in these forums:
Black Hole Complementarity
Leonard Susskind, THE BLACK HOLE WAR (his arguments with Stephen Hawking) (p238) Today a standard concept in black hole physics is a stretched horizon which is a layer of hot microscopic degrees of freedom about one Planck length thick and a Planck length above the event horizon. Every so often a bit gets carried out in an evaporation process. This is Hawking radiation. A free falling observer sees empty space.

(p258) From an outside observer’s point of view, an in falling particle gets blasted apart….ionized….at the stretched horizon…before the particle crosses the event horizon. At maybe 100,000 degrees it has a short wavelength and any detection attempt will ionize it or not detect it!

(p270)…. eventually the particle image is blurred as it is smeared over the stretched horizon and….and the image may (later?) be recovered in long wavelength Hawking radiation.

I saved this very concise explanation of the other two thus: {did not record the author}

"horizon" you mean "absolute horizon", i.e., the boundary of the region from which light signals cannot escape to infinity. However, this is *not* the same as an "apparent horizon", which is a "trapped surface" at which outgoing light signals no longer move outward.
When the absolute horizon first forms at the center of the gravitating body, there is no apparent horizon; outgoing light rays are still moving outward.

The apparent horizon is a local (instantaneous, discontinuous) phenomenon...It would not seem to have any
dimension. The absolute horizon (continuous, forms at the center of mass and moves outward) is global...not likely it has a dimension either.

And another related phenomena is the photon sphere. The position of the photon sphere is the apparent dividing line between black hole and sky..outside the event horizons.
Wiki is down right now, but I know it is discussed there. I am not positive if this is considered a 'horizon'; I think not but am unsure exactly why.

Physicsforums has a description...looks like it has no 'thickness'??
https://www.physicsforums.com/library.php?do=view_item&itemid=268
 
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Naty1 said:
a related feature is that everytime a larger horizon is envisioned, it too encapsulates all the interior information...in other words every time you look at a larger horizon all the information is THERE...

And this gets weird when you have a cosmic event horizon. Once dark energy pushs a galaxy through the cosmic horizon then all of information is still there.
 
  • #11
twofish-quant said:
And this gets weird when you have a cosmic event horizon. Once dark energy pushs a galaxy through the cosmic horizon then all of information is still there.

yes!
Apparently even the Hubble sphere is an event horizon of sorts {despite repeated earlier claims in these forums that it is not} from which :

Authors:T. Padmanabhan
(Submitted on 2 Jul 2012)
Abstract: ... In the second part, I describe a novel way of studying cosmology in which I interpret the expansion of the universe as equivalent to the emergence of space itself. In such an approach, the dynamics evolves towards a state of holographic equipartition, characterized by the equality of number of bulk and surface degrees of freedom in a region bounded by the Hubble radius.

Gravity appears to make horizon entropy finite. Space, time and quantum fluctuations in his perspective emerge from thermodynamic degrees of freedom considerations: Because the Hubble Horizon limits degrees of freedom, a symmetry which I suppose of a vacuum that is broken, 'stuff' becomes emergent! Another way to say this, I think, is that analogous to GR where geometry creates gravity, a thermodynamic 'equipartition' view can show expanding geometry spawns particles.

Feynman says "The truth is always simpler than you thought."
I have not yet gotten THAT far!
 
  • #12
many thanks to @marcus,@Naty1 and @twofish-quant,
im very happy that there is a lot of "strangeness" there,and your insights have pointed me in many areas to explore.
thanks to your specifications i have much much food for thought!
i have found a set of lectures covering this topic by Leonard Susskind,though the title is misleading(topics in string theory)it covers exactly the very features of interest that you guys described.
There are 9 lectures,im only about 2 lectures in,and there's lots of areas of maths that i have to learn as i go along,so i had better settle down for a while.
You guys are great! Horizons are great, and I am going to start to learn physics which i should have done years ago
thanks again
 
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