Why is Hawking Radiation Necessary for Black Hole Evaporation?

In summary, according to the theory, a particle anti particle pair are formed, and rather than colliding within a given period of time (dictated by the heisenburg uncertainty principle), in order to prevent the violation of conservation of mass, one of the particles falls into the black hole. According to wikipedia- the pair's creation (instantaneous) and annihilation (immediate) is necessary for the black hole to evaporate.
  • #1
roundedge
8
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I'm having trouble understanding why it is necessary for there to be a particle antiparticle pair formation in order for the black hole to evaporate.

According to my understanding of the theory, a particle anti particle pair are formed, and rather than colliding within a given period of time (dictated by the heisenburg uncertainty principle), in order to prevent the violation of conservation of mass, one of the particles falls into the black hole. According to wikipedia-

"In order to fill the energy 'hole' left by the pair's spontaneous creation, energy tunnels out of the black hole and across the event horizon. By this process the black hole loses mass, and to an outside observer it would appear that the black hole has just emitted a particle."

My first question is, what was preventing the energy from tunneling out of the black hole in the first place? I mean, isn't quantum tunneling simply a matter of probability? Say you have two states, the inside of the event horizon, and the outside of the event horizon. Treat the system as an energy hill, like an activation energy in chemistry, except the hill is infinitely high, which is why nothing can escape a black hole in classical physics. However, according to the theory of quantum physics, it's merely a matter of probability that the subject exists in one state, and not the other, so there is a chance that the subject could "tunnel", or appear, on the other side of the event horizon.

My second question is, does the energy disappear? Say an anti proton falls into the black hole, and a proton escapes the event horizon. The black hole then parcels out some amount of energy equivalent to the combined mass of both the particle and the anti particle, and that energy disseapears from the black hole, such that, not only has the gain in energy from the anti proton falling in been negated, but also an amount of energy has been lost equivalent to the proton being "emited". But where does that energy go?

I suspect there's something crucial missing in my understanding of the instantaneous creation and anihalation of particle anti particle pairs. Any help?
 
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  • #2
roundedge said:
My second question is, does the energy disappear? Say an anti proton falls into the black hole, and a proton escapes the event horizon. The black hole then parcels out some amount of energy equivalent to the combined mass of both the particle and the anti particle, and that energy disseapears from the black hole, such that, not only has the gain in energy from the anti proton falling in been negated, but also an amount of energy has been lost equivalent to the proton being "emited". But where does that energy go?

I suspect there's something crucial missing in my understanding of the instantaneous creation and anihalation of particle anti particle pairs. Any help?
I agree - this is something I also never understood about Hawking radiation. The simplistic description in terms of particle-anti-particle pair creation would seem to imply that the in-falling particle has "negative mass-energy" :eek: (otherwise the Black Hole would gain mass instead of losing mass).

In fact, Hawking himself describes it in just this way in Chapter 7 of his book A Brief History of Time :

Hawking said:
Because energy cannot be created out of nothing, one of the partners in a particle/antiparticle pair will have positive energy, and the other partner negative energy.

see the chapter here : http://www.physics.metu.edu.tr/~fizikt/html/hawking/f.html

I suspect the error is in the simplistic interpretation in terms of particle-anti-particle pair creation.

Can anyone shed light on this?

Best Regards
 
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  • #3
I think is the moot point:

"So in empty space the field cannot be fixed at exactly zero, because then it would have both a precise value (zero) and a precise rate of change (also zero). There must be a certain minimum amount of uncertainty, or quantum fluctuations, in the value of the field. One can think of these fluctuations as pairs of particles of light..."

You can think of them as particles. But they're fluctuations rather than "billiard ball" particles.
 
  • #5
Thanks for that, George. I wasn't clear on why the Black Hole can swallow a negative half of a "virtual particle pair" leaving the positive half free to radiate, but not vice versa:

Note that this doesn't work in the other direction - you can't have the positive-energy particle cross the horizon and leaves the negative-energy particle stranded outside, since a negative-energy particle can't continue to exist outside the horizon for a time longer than h/E. So the black hole can lose energy to vacuum fluctuations, but it can't gain energy.

Can you or anybody else rephrase this?
 
  • #6
Farsight said:
Thanks for that, George. I wasn't clear on why the Black Hole can swallow a negative half of a "virtual particle pair" leaving the positive half free to radiate, but not vice versa:

Note that this doesn't work in the other direction - you can't have the positive-energy particle cross the horizon and leaves the negative-energy particle stranded outside, since a negative-energy particle can't continue to exist outside the horizon for a time longer than h/E. So the black hole can lose energy to vacuum fluctuations, but it can't gain energy.

Can you or anybody else rephrase this?


That seems like a bit of a cop out explanation. It's almost just saying "the anti particle can't exist outside of the event horizon, because it's just not aloud" The fundamental process, according to my understanding, is as simple as one crossing the event horizon, and the other not. The process makes no distinction between a particle or an anti particle. The only way I could imagine there being a distinction made is if one of the particles were gravitationally repulsive. But it would be the regular particle which would have to be gravitationally repulsive in order for it to always be outside of the event horizon, and we all know that conventional matter is gravitationally attractive.
 
  • #7
George Jones said:
You might want to read Steve Carlips's exposition of Hawking radiation, to which I gave a link in a https://www.physicsforums.com/showpost.php?p=620350&postcount=4".
Thanks, interesting link, but I'm still confused. The last paragraph just doesn't seem explicable :

you can't have the positive-energy particle cross the horizon and leaves the negative-energy particle stranded outside, since a negative-energy particle can't continue to exist outside the horizon for a time longer than h/E.
This simply states that the positive energy particle cannot cross the event horizon - it does not explain WHY it cannot cross the event horizon. What prevents it?

I've also come across this weird paper :

http://arxiv.org/PS_cache/hep-th/pdf/0402/0402145.pdf

which suggests that black holes do NOT in fact evaporate, but they simply accumulate "negative energy" as they radiate :

The black hole mass eventually drops to zero in semiclassical gravity, but this semiclassical state has an infinite temperature and still contains all the initial matter together with the negative energy entangled with the exterior radiation.
?
 
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  • #8
Further problems trouble me with Hawking Radiation, as follows :

(1) The HUP says that the particle-anti-particle pair will exist for a maximum time t given by

t = h/(4.Pi.E)

where E is the total energy of the pair. If one particle has negative energy and the other has positive energy, then surely the total energy of the pair could be zero, hence the pair could continue to exist indefinitely... ?


(2) The energies involved in Hawking radiation are so small (for massive black holes) that the radiation is most likely to be in the form of photons. The energy of a photon is simply related to it's frequency (f) as follows :

E = h.f

Thus the HUP-lifetime of a pair of virtual photons (if we consider them both to have positive energy) is given by :

t = 1/(8.Pi.f)

In other words, the HUP-lifetime will be approximately 4% of the time required for the photons to "exist for one wavelength". These virtual photons therefore pop into, and out of, existence in (at most) 4% of their wavelengths...

weird?
 
  • #9
I doubt the radiation is in the form of photons

I don't think there's such thing as a photon/anti-photon pair
 
  • #10
roundedge said:
I doubt the radiation is in the form of photons

I don't think there's such thing as a photon/anti-photon pair

The photon is its own antiparticle.
 
  • #11
selfAdjoint said:
The photon is its own antiparticle.
Yep.

For a black hole with mass the same as earth, the event horizon would have a radius of just 8.9mm, and would emit Hawking radiation with frequency around 1.35Ghz (similar in frequency to the radio waves used in mobile phones). This corresponds to an energy of approx 5.6 x 10^-6 eV.

The rest mass of an electron is 5.1 x 10^5 eV - almost one trillion times more than the above Hawking radiation energy. Only some neutrinos, gravitons (if they exist) and photons, are less massive than the electron (in fact photons and gravitons are massless).

Thus the only known way that a black hole with the mass of the Earth could emit Hawking radiation would be in the form of either photons, some neutrinos, or gravitons (and gravitons I'm not sure about).

More massive black holes would emit even lower energy radiation.

Best Regards

see : http://library.thinkquest.org/C007571/english/advance/english.htm
 
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  • #12
moving finger said:
The rest mass of an electron is 5.1 x 10^5 eV - almost one trillion times more than the above Hawking radiation energy. Only some neutrinos, gravitons (if they exist) and photons, are less massive than the electron (in fact photons and gravitons are massless).
Actually, it's even worse than I suggested.

For any particle to be emitted as Hawking radiation, the particle would need to have a velocity close to the speed of light in order to ensure it did not get sucked back into the black hole. For any particle with non-zero rest mass this implies a total energy far in excess of its rest mass

Best Regards
 
  • #13
I think the reason why it is always given that the black hole absorbs the negative energy is because the particle/antiparticle pairs are entangled. Hence, one half of the entangled pair crosses the horizon while the other propagates out into space. If the "free" half of the pair is detected then it will give a positive energy in the detector meaning that the other particle has negative energy.
 
  • #14
MaverickMenzies said:
I think the reason why it is always given that the black hole absorbs the negative energy is because the particle/antiparticle pairs are entangled. Hence, one half of the entangled pair crosses the horizon while the other propagates out into space. If the "free" half of the pair is detected then it will give a positive energy in the detector meaning that the other particle has negative energy.
I don't think it's that simple. If one half of an entangled pair has negative energy then the total energy of the pair will be zero and the permitted lifetime (t) of that virtual pair will be infinite, by the Heisenberg Uncertainty Principle :

t = h/(4.Pi.E)

where E is the total energy of the pair.

The only reason that virtual particle pairs have very short lifetimes (which we can calculate using the above equation) is because the total energy of the pair is positive.

Best Regards
 
  • #15
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  • #16
There was a previous thread about HR, and one of the staff (Maybe Doc Al? Or Mentz... I forget) pointed out that this really takes specialized math and lectures to grasp. The concept as it is usually disseminated (particle/anti-particle fail to annihilate) isn't wrong per se, but it's not right either. This is just one of the very VERY technical theories out there, and one which is still being developed.
 

1. Why is Hawking Radiation necessary for black hole evaporation?

Hawking Radiation is necessary for black hole evaporation because it is the only known process by which black holes can lose mass and energy. Without this radiation, black holes would continue to grow in size and mass, making them even more powerful and dangerous.

2. How does Hawking Radiation contribute to black hole evaporation?

Hawking Radiation is created when virtual particles near the event horizon of a black hole become separated, with one particle being pulled into the black hole and the other escaping. This escaping particle carries away energy from the black hole, causing it to gradually lose mass and eventually evaporate.

3. Can black holes evaporate without Hawking Radiation?

No, black holes cannot evaporate without Hawking Radiation. This is because Hawking Radiation is the only known process by which black holes can lose mass and energy. Without this radiation, black holes would continue to grow in size and mass, making them even more powerful and dangerous.

4. How does Hawking Radiation affect the size and lifespan of black holes?

Hawking Radiation causes black holes to gradually lose mass and energy, which in turn affects their size and lifespan. As a black hole loses mass, its gravitational pull becomes weaker and it eventually evaporates completely. This process can take trillions of years for a supermassive black hole, but much less time for smaller black holes.

5. Is Hawking Radiation the only factor in black hole evaporation?

No, there are other factors that can contribute to black hole evaporation, such as the emission of other types of radiation and the effects of quantum mechanics. However, Hawking Radiation is currently believed to be the most significant factor in the evaporation of black holes.

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