Skip to the Main Content

Note:These pages make extensive use of the latest XHTML and CSS Standards. They ought to look great in any standards-compliant modern browser. Unfortunately, they will probably look horrible in older browsers, like Netscape 4.x and IE 4.x. Moreover, many posts use MathML, which is, currently only supported in Mozilla. My best suggestion (and you will thank me when surfing an ever-increasing number of sites on the web which have been crafted to use the new standards) is to upgrade to the latest version of your browser. If that's not possible, consider moving to the Standards-compliant and open-source Mozilla browser.

March 14, 2005

The Blackhole of Chapline

Imagine that 2 million light years from our current location is a collapsing shell of radiation, headed towards us. Two million years from now (minus a little bit) that shell will pass within its Schwarzschild radius and a blackhole will reside where we once stood.

But we don’t know that yet. We can’t know that yet. The shell of radiation is well outside our past lightcone. Still, despite our blissful ignorance of the doom that awaits us, an event horizon has already formed here on Earth. Light signal from our present location will never escape to infinity. The existence of this event horizon is a global geometrical statement. When, exactly, it formed depends on the total “mass” of that shell of radiation. And … we don’t know what that is.

Penrose diagram for a collapsing shell of radiation
Penrose diagram for a blackhole formed by a collapsing shell of radiation. The horizon forms before any knowledge of the collapsing shell reaches the hapless observer.

For you and me, the horizon is undetectable. There are no local measurements that we can make that will allow us to determine whether the statements of the first paragraph of this essay are correct.

George Chapline, of Livermore National Lab (along with his apparent partner in crime, Bob Laughlin), however, can tell. He claims that when you and I cross the horizon, we can observe all sorts of weird quantum-mechanical phenomena. And the thickness of the region over which these phenomena take place is a function of the mass of the blackhole that will ultimately form.

George’s chums in the Andromeda galaxy can send him superluminal signals by manipulating the “strength” of that collapsing shell (and hence the size of the region over which one observes this quantum criticality).

Normally, I wouldn’t belabour this sort of thing. But I just sat through a Harvard Physics Colloquium by the aforementioned gentleman. It was the most surreal hour I ever spent in Jefferson Laboratory.

Luboš, in his own inimitable style, has more to say on the subject.

Posted by distler at March 14, 2005 8:40 PM

TrackBack URL for this Entry:   https://golem.ph.utexas.edu/cgi-bin/MT-3.0/dxy-tb.fcgi/530

15 Comments & 1 Trackback

Re: The Blackhole of Chapline

Just to play devil’s advocate, what if you replaced `event horizon’ by `apparent horizon’?

Posted by: Aaron Bergman on March 14, 2005 10:19 PM | Permalink | Reply to this

Apparent Horizon

The apparent horizon, at least, can be defined by a local criterion. So the assertion that something funny happens there is not prima facie absurd.

Altering the known laws of physics at the apparent horizon would be pretty radical in itself. But he wants to fix the “paradoxical” behaviour of blackholes. That ambitious goal requires that something funny happen at the event horizon.

Posted by: Jacques Distler on March 14, 2005 10:41 PM | Permalink | PGP Sig | Reply to this

Re: Apparent Horizon

On the other hand, we believe in things like unitarity and Hawking radiation which all seem to indicate that something funky is going on somewhere.

Mathur, if you believe him, has the horizon never forming, so something must happen to your sphere of infalling dust.

And, because it’s late at night and I have a cold, I can make half-assed guesses. Assuming you don’t mess with the GR lagrangian too much and you believe the null energy condition (both of which have issues, I suppose), then you better not ever create a trapped surface. Being about to create a marginally trapped surface seems to me to be as good a guess for a local criterion as any.

Posted by: Aaron Bergman on March 15, 2005 12:55 AM | Permalink | Reply to this

Re: The Blackhole of Chapline

Jacques,

I completely agree with your picture and conclusion but I would like to point out two issues with your configuration:
1) In order to make your point you require “sharp” edges of your shell which would result in discontinuities.
2) the asymptotics of your example is a bit funny (your space is not flat at infinity)

Best,
Wolfgang

Posted by: Wolfgang on March 15, 2005 8:07 AM | Permalink | Reply to this

Edges

  1. We could smooth the edges of the shell so that the leading edge (observable today) is weaker than the background radiation impinging on the earth.
  2. I only had the shell extending out to past null-infinity to ensure that it could never have been in causal contact with us today. Alternatively, it could have been created yesterday by Chapline’s chums in the Andromeda Galaxy. If our telescopes were sufficiently powerful, we would be able to observe their arboreal ancestors coming down from the trees, and know that, in the future, their descendants would construct a “Doomsday Machine” and train it upon us.

I leave it you you to decide whether that modified scenario should induce quantum criticality here today.

Posted by: Jacques Distler on March 15, 2005 9:09 AM | Permalink | PGP Sig | Reply to this

Re: The Blackhole of Chapline

Now I’m not a hot-shot physicist like all of you (in fact, I haven’t even passed Quantum Mechanics 1 yet), so excuse my ignorance please.

If an event horizion formed and Chapline’s friends in Andromeda can send him a FTL signal warning him, why can’t he start an explosion, change the distribution of energy inside shell (altering how it collapses) or do something that causes the singularity not to form in a million or so years? There’s probably something I’m missing.

Posted by: Jimmy Cerra on March 15, 2005 2:37 PM | Permalink | Reply to this

Spelling it out

You have, indeed, discovered one of the many, many reasons why any theory that allows faster-than-light signalling is necessarily crap.

Thanks for spelling that out. As a “hot shot physicist,” I tend to assume that as soon as I explain that “X implies faster-than-light signalling”, my audience immediately apprehends the implication that “X is utter crap”.

Posted by: Jacques Distler on March 15, 2005 2:51 PM | Permalink | PGP Sig | Reply to this

Re: Spelling it out

What about quantum entanglement? Doesn’t this qualify as FTL communications?

Posted by: Le Snelson on April 29, 2005 3:23 PM | Permalink | Reply to this

Entanglement

Nope.

Entanglement ≠ Communication. You can prove that no information gets transmitted that way; i.e., you can’t use quantum entanglement for signalling.

Posted by: Jacques Distler on April 29, 2005 4:39 PM | Permalink | PGP Sig | Reply to this

Re: The Blackhole of Chapline

“I tend to assume that as soon as I explain that “X implies faster-than-light signalling”, my audience immediately apprehends the implication that “X is utter crap”.”

Another diagnostic of Utter Crap is when the author of a paper writes that future historians will look back at his work as a turning point in the history of physics, as Chapline does. Sad.

Posted by: Serenus on March 16, 2005 2:42 AM | Permalink | Reply to this

Re: The Blackhole of Chapline

Er, I am not sure, but it feels as if FTL signaling and “future historians” in a same paper are in some sense meta-inconsistent concepts.

Posted by: Alejandro Rivero on March 16, 2005 7:22 AM | Permalink | Reply to this

Re: The Blackhole of Chapline

Quick diagram question, how fast does gravity travel in your scenario?

Posted by: Ripper on April 2, 2005 6:41 AM | Permalink | Reply to this

Penrose diagrams

I’m not sure I understand your question, but let me try to answer it anyways.

In a Penrose diagram, light (or, indeed, any massless propagating field, like gravitational waves) travels along 45° lines.

Massive particles propagate vertically, or, at least, at angles less than 45° from vertical.

“Past null-infinity” is the 45° line at the lower right of the figure. Signals can propagate in from there. “Future null-infinity” is the 45° line at the upper right. Signals can propagate out to there.

But there’s a region of spacetime (to the upper left of the dashed line marked “event horizon”) which cannot send signals out to future null-infinity. Indeed, that’s what the event horizon means It separates regions of spacetime which can send signals out to future null-infinity from those which can’t.

Posted by: Jacques Distler on April 2, 2005 10:50 AM | Permalink | PGP Sig | Reply to this

Re: The Blackhole of Chapline

Nature reports that black holes ‘do not exist’:

George Chapline thinks that the collapse of the massive stars, which was long believed to generate black holes, actually leads to the formation of stars that contain dark energy. “It’s a near certainty that black holes don’t exist,” he claims.

Posted by: Volker Braun on April 4, 2005 9:59 AM | Permalink | Reply to this

That old rag?

I think we have all learned that nothing published in Nature on the subject of physics should be assumed to be trustworthy.

Posted by: Jacques Distler on April 4, 2005 4:47 PM | Permalink | PGP Sig | Reply to this
Read the post Camino 1.0
Weblog: Musings
Excerpt: ... and it finally supports MathML.
Tracked: July 6, 2007 5:36 PM

Post a New Comment