Physicists propose experiment to see the ‘grin’ of quantum gravity
quantamagazine.org
quantamagazine.org
https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.11...
https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.11...
One challenge, which is commonly a problem for laboratory gravitational experiments, is that many other force interactions dominate over short distance scales (electric, magnetic, or even vibrational phonons) so excluding those is critical to showing the entanglement is gravitational. This means near perfect electrical, magnetic, and vibrational isolation... and probably measuring their coupling amplitude them to show that it is perfect.
As usual in experimental physics, the problem is not in detecting the effect, but in not detecting all the other interfering effects. It borders on proving a negative.
I imagine there is some context for this question, but I can not really give a better answer without knowing the question. My guess is that the question stems from a misunderstanding what a graviton is, so I will grossly simplify and say: graviton is to gravitational field what photon is to electrostatic field.
Gravity at black holes’s event horizon is not quite coming from where you think it is: it isn’t ”emitted by” or ”emanating from” the singularity. Rather, as gravity is a form of energy, and mass-energy creates gravity, the gravitational field at the border, within our observable universe, is intense enough to whip itself up into a self-maintaining recursive but sustainable loop. No communication from what lies within the event horizon is neither possible nor required.
I still don't quite get "the gravitational field at the border, within our observable universe, is intense enough to whip itself up into a self-maintaining recursive but sustainable loop" (especially the self-maintaining, recursive part. How?), but I guess one would need a good understanding of GR to go beyond this level?
"[...] the electromagnetic repulsion or attraction between two charges—can be thought of as due to the exchange of many virtual photons between the charges."
so when the electromagnetic force mediation takes place, it exchanges virtual photons, and this is different from an object exchanging physical photons with another (which we would more think of as one object shining (if the photon is in the visible spectrum) on another).
How a virtual graviton would interact between BHs and other particles are up to any suggested theory for quantum gravity to explain.
http://math.ucr.edu/home/baez/physics/Relativity/BlackHoles/... https://www.quora.com/in/If-both-the-photon-and-the-graviton...
What I am trying to describe is the inherent nonlinearity of general relativity, wherein compound solutions cannot be obtained simply summing up or overlaying simpler situations: the gravity filed itself generates more gravity, so it can recursively reach and sustain a critical value.
The Higgs does not play that kind of role. It is a common misconception, since Higgs it often referred to as "giving mass to the other particles", which is true, and called the Higgs-mechanism, it does not influence the curvature of space-time that way. That is all due to the graviton (assuming, which it is also commonly believed, that gravity is quantised).
Mass is one thing, interactions between masses another.
This is a non sequitur, presumably due to a misunderstanding caused from some pop sci article. You really do not need gravitons to describe any of the dynamics of "pulling matter in" (at least for "usual" black holes), and there is no "pushing out gravitons" involved.
In perturbatively quantized gravity, we start with a background metric (e.g. Minkowski flat spacetime or Schwarzschild black hole spacetime) and then "perturb" it with other moving matter. With a careful choice of slicing of the 4-spacetime into 3+1 space+time, we can see the (leading order) deviations from the background metric as a plane wave propagating lightlike from one spacelike slice to the next. Quantizing those waves in much the same way as we quantize classical electromagnetic planar waves leads to the graviton as a massless boson (but with spin-2 instead of spin-1).
A spherically symmetric non-rotating black hole (and having factored out changes in coordinate position and linear momentum by choice of coordinates) sources exactly the Schwarzschild metric, so there is no perturbation from a Schwarzschild background (and thus no gravitational waves to quantize, and thus no gravitons in the vincinity). If we throw something into it, there will be a perturbation of the exterior metric, and thus gravitons in principle observable outside the horizon.
There are theories that define a graviton, and the result ought to be the same: you generally only get (real rather than virtual) gravitons when something is falling into a (maximally symmetric) black hole (and very shortly afterwards, during "balding"), or:
If you break the Schwarzschild symmetries by adding angular momentum and/or charge to the black hole, you can also get perturbations of a well-chosen background metric, although extremely little gravitational radiation (and thus few gravitons) unless something massive is sufficiently near the black hole.
But just to repeat: an isolated non-rotating black hole emits no gravitons. You need to perturb it out of its highly symmetrical state in order to get gravitons. [cf. https://en.wikipedia.org/wiki/Gravitational_wave?oldformat=t... -- for a black hole the relevant configurations are a significant "bump" on an otherwise highly symmetric black hole or a significant mass creating a "barbell" style binary]
Those previous HN submissions don't count as dupes because they didn't get significant attention. This is in the FAQ: https://news.ycombinator.com/newsfaq.html.
My question why is it getting so long to get result How do software step in to help streamline research ? I can not help thinking this is steve job 'next' company time in the sun