| Detecting Quantum Spacetime 
By Marcus ChownNew Scientist, January 15, 2009
 
	Edited by Andy Ross 
	The Anglo-German GEO600 experiment is looking for gravitational waves from 
	super-dense astronomical objects such as neutron stars and black holes. 
	GEO600 has not detected any gravitational waves so far, but it might 
	inadvertently have made the most important discovery in physics for half a 
	century.
 According to Craig Hogan, a physicist at Fermilab, GEO600 
	has stumbled upon the fundamental limit of spacetime: "It looks like GEO600 
	is being buffeted by the microscopic quantum convulsions of spacetime. If the GEO600 result is what I suspect it is, then we are all 
	living in a giant cosmic hologram."
 
 In the 1990s physicists Leonard 
	Susskind and Gerard 't Hooft suggested that the 3D world of our everyday 
	experience might be a holographic projection of physical processes that take 
	place on a distant, 2D surface.
 
 This idea arose from work by Jacob 
	Bekenstein of the Hebrew University of Jerusalem and Stephen Hawking at the 
	University of Cambridge. Hawking had shown that black holes emit radiation. 
	When the black hole evaporates, all the information about the star that 
	collapsed to form it vanishes, which contradicts the principle that 
	information cannot be destroyed. This is known as the black hole information 
	paradox.
 
 Bekenstein discovered that a black hole's entropy is 
	proportional to the surface area of its event horizon. Theorists have since 
	shown that microscopic quantum ripples at the event horizon can encode the 
	information inside the black hole, so there is no mysterious information 
	loss as the black hole evaporates.
 
 Crucially, the 3D information 
	about a precursor star can be completely encoded in the 2D horizon of the 
	subsequent black hole. Susskind and 't Hooft extended the insight to the 
	universe on the basis that the cosmos has a horizon too. Juan Maldacena at 
	the Institute for Advanced Study, Princeton, has shown that the physics 
	inside a 5D hyperbolic universe is the same as the physics on its 4D 
	boundary.
 
 Physicists have long believed that quantum effects will 
	cause spacetime to convulse wildly on the tiniest scales. At the Planck 
	scale, spacetime is made of units rather like pixels with a size of 10—35 
	m.
 
 If spacetime is a grainy hologram, then you can think of the 
	universe as a sphere covered in Planck-sized tiles, each containing one bit 
	of information. The holographic principle says the number of Planck tiles 
	must match the number of bits in the universe.
 
 But the volume of the 
	sphere is much bigger than its outer surface. Hogan realized that the world 
	inside must be made up of grains bigger than the Planck length. So while the Planck 
	length is too small for experiments to detect, the holographic projection 
	of that graininess could be much larger, at around 10—16 m.
 
 Gravitational wave detectors measure length. If a 
	gravitational wave passes through GEO600, it will alternately stretch space 
	in one direction and squeeze it in another. To measure this, the GEO600 team 
	fires a laser through a beam splitter. The two beams pass down the 
	instrument's 600-m perpendicular arms and bounce back again. The returning 
	beams merge again at the beam splitter and create an interference pattern. 
	Any shift in the pattern shows that the relative lengths of the arms has 
	changed.
 
 Hogan predicted that if the GEO600 beam splitter is buffeted by the quantum 
	jitters of spacetime, this will show up as noise in its measurements 
	(Physical Review D, v77, p104031).
 
 In June 2008, Hogan sent his 
	prediction to the GEO600 team and discovered that the experiment was picking 
	up unexpected noise. GEO600 principal investigator Karsten Danzmann of the 
	Max Planck Institute for Gravitational Physics, Potsdam, and the University 
	of Hanover, says the excess noise, with frequencies of between 300 and 1500 
	Hz, had been bothering the team.
 
 Gravitational-wave detectors are extremely sensitive. 
	"The daily business of improving the sensitivity of these experiments always 
	throws up some excess noise," says Danzmann. He says planned upgrades should 
	improve the sensitivity of GEO600 and eliminate some possible sources of 
	noise. "If the noise remains where it is now after these measures, then we 
	have to think again," he says.
 
 It would be ironic if an instrument 
	built to detect astrophysical sources of gravitational waves inadvertently 
	detected the quantum graininess of spacetime. Danzmann: "It would be 
	one of the most remarkable discoveries in a long time."
 
	AR  Wonderful discovery! If 
	this really does turn out to be quantum jitters, the event is as momentous 
	as the discovery of the cosmic microwave background.
 Toward Quantum Gravity 
By Anil AnanthaswamyNew Scientist, August 12, 2009
 
	Edited by Andy Ross 
	Physicists have been on the lookout for signposts to the right theory of 
	quantum gravity for the best part of a century.
 "All approaches to 
	quantum gravity, in their own very different ways, agree that empty space is 
	not so empty after all," says theorist Giovanni Amelino-Camelia of Sapienza 
	University of Rome in Italy. Many models based on string theory suggest that 
	spacetime is a foamy froth of particles that appear out of nothing and 
	disappear again with equal abandon. The alternative approach, loop quantum 
	gravity, posits that spacetime comes in tiny chunks.
 
 Last year, the 
	signature of quantum spacetime may have popped up in unexplained noise in a 
	gravity-wave detector in northern Germany. But most experts agree that a 
	more substantive sighting could only come from observing the possible 
	interactions of spacetime with particles passing through it.
 
 According to many string theory models, particles of different energies 
	should speed up or slow down by different amounts as they interact with a 
	foamy spacetime. A minimum size for spacetime grains, as predicted by loop 
	quantum gravity, could violate Lorentz invariance, which states that the 
	maximum speed of all particles is the speed of light in a vacuum.
 
 As 
	yet, we have only seen a handful of gamma-ray bursts of the energy and 
	intensity needed to see whether the delay effect is a consistent feature. 
	The uncertainties in the data make a definitive statement impossible.
 
 In September 2008, the NASA Fermi Gamma-ray Space Telescope detected a 
	burst of gamma rays from a source nearly 12 billion light years away. At 
	CERN, John Ellis and colleagues used a theoretical model that assumes the 
	delay effect increases linearly with distance and photon energy to estimate 
	the delay that the highest-energy photon in the Fermi burst should have 
	experienced. They came up with 25 s, plus or minus 11 s, 
	compared with a measured 16.5 s.
 
 The only way to find out 
	conclusively whether the delays are a consistent signature of quantum 
	spacetime is to get more data. Combining different data sets will provide a 
	wider spread of energies from which to tease out any energy-dependent 
	effect, and also overcome the fact that Earth's rotation makes observing a 
	highly directed beam of gamma rays from one direction tricky.
 
 The new 
	gamma ray telescopes could well uncover quantum spacetime within the next 
	few years. Or the answer might come from a cubic kilometre of ice under the 
	South Pole, home to the IceCube Neutrino Observatory, whose strings of 
	detectors will watch for faint flashes of blue light emitted when neutrinos 
	from cosmic sources smash into the Antarctic ice.
 
 Neutrinos are 
	thought to be produced in the same violent events that produce high-energy 
	gamma rays. As yet, we have seen hardly any neutrinos from outside our 
	galaxy. The neutrinos we see are lower-energy ones that come from nuclear 
	reactions in the sun and particle interactions in Earth's atmosphere. 
	IceCube aims to change that.
 
 Because the wavelengths associated with 
	neutrinos of the very highest energies are even smaller than those of 
	high-energy photons, they could be more susceptible to disruption through 
	interactions with a spacetime that is grainy on very small scales. Francis 
	Halzen of the University of Wisconsin, Madison, who leads the IceCube 
	experiment, has calculated with his colleagues that in one model of quantum 
	spacetime such interactions could dramatically speed up higher-energy 
	neutrinos.
 
 Neutrinos come in three distinct flavors: the electron, 
	the muon, and the tau. They tend to oscillate back and forth between these 
	flavors as they travel. If a distant source is emitting only electron 
	neutrinos, theory tells us how many should have changed flavor by the time 
	they reach us. If neutrinos were interacting with the quantum foam, they 
	would forget their original flavor along the way, leading to equal numbers 
	of all flavors by the time they arrive here.
 
 Even if we find 
	indisputable signs that either neutrinos or gamma rays are being affected by 
	the structure of spacetime, it will be hard work to convert that evidence to 
	support for a viable theory of quantum gravity.
 
	AR  We have a way to go, sure, 
	but the picture looks good: spacetime is quantized somehow.
 Breaking Lorentz Symmetry 
By 
Anil AnanthaswamyNew Scientist, August 9, 2010
 
	Edited by Andy Ross 
	Petr Horava wants to rip time and space free from one another in a unified 
	theory that reconciles quantum mechanics and gravity.
 For decades now, physicists have 
	tried to reconcile Einstein's general theory of relativity and quantum 
	mechanics. The stumbling block lies with their conflicting views of space 
	and time. As seen by quantum theory, space and time are a static backdrop 
	against which particles move. In Einstein's theories, by contrast, space and 
	time form a spacetime continuum that is curved by the bodies within it.
 
 We need to marry relativity and quantum theory to understand what 
	happened just after the big bang or what's going on near black holes, where 
	the gravitational fields are immense. The problem comes to the fore in the 
	gravitational constant G. On large scales, the equations of general 
	relativity yield a value of G that tallies with observed behavior. But at 
	very small distances, quantum fluctuations of spacetime ruin any calculation 
	of G.
 
 Looking for a way out, Horava found inspiration in the physics 
	of condensed matter. Graphene is a sheet of carbon atoms just one atom 
	thick. The motion of the electrons in the sheet can be described using 
	quantum mechanics, and because they are moving at only a small fraction of 
	the speed of light there is no need to take relativistic effects into 
	account.
 
 But cool graphene down to near absolute zero and the 
	electrons speed up dramatically. Now relativistic theories are needed to 
	describe them correctly. In relativity, spacetime has Lorentz symmetry: to 
	keep the speed of light constant for all observers, time slows and distances 
	contract in exact proportion.
 
 Lorentz symmetry isn't always apparent 
	in graphene. In our universe, space and time appear linked by Lorentz 
	symmetry. But the symmetry may have emerged as the universe cooled from the 
	big bang fireball, just as it emerges in graphene when it is cooled.
 
 So Horava changed Einstein's equations in a way that removed Lorentz 
	symmetry. This led to equations that describe gravity in the same quantum 
	framework we use fo the other forces. He also made another change. 
	Einstein's theory does not have an arrow of time, but the universe as we 
	observe it does. Horava gave time a preferred direction and found that 
	quantum field theories could then describe gravity at microscopic scales 
	without producing nonsense (Physical Review D, v79, p084008).
 
 An 
	approach to quantum gravity called causal dynamical triangulation stitches 
	spacetime together from smaller pieces. 
	Jan Ambjørn of the Niels Bohr 
	Institute in Copenhagen, Denmark, and his colleagues, used computer 
	simulations to analyze spacetime and found that space and time varied in a 
	strange way. Zoom out and space and time obey Lorentz symmetry. But zoom in 
	and time plays a far greater role than space. Ambjørn thinks Lorentz 
	symmetry may be broken as in Horava gravity (first abstract below).
 
 Horava gravity has already been used to study black holes, dark matter, and 
	dark energy. In general relativity, black holes appear when the curvature of 
	spacetime increases without limit. By breaking the symmetry between space 
	and time, Horava's theory alters the physics of black holes in ways that are 
	still unknown.
 
 Horava gravity might also help with the long-standing 
	puzzle of dark matter. Shinji Mukohyama at the University of Tokyo extracted 
	the equations of motion from Horava's theory and found that they allow 
	something like dark matter (second abstract below).
 
 Dark energy is 
	more daunting. The theories of particle physics predict the strength of dark 
	energy to be about 120 orders of magnitude larger than what is observed. 
	Horava's theory contains a tunable parameter that can reduce the prediction 
	to a realistic value (third abstract below).
 
 
	CDT meets Horava-Lifshitz gravityJ. Ambjørn, A. 
	Gorlich, S. Jordan, J. Jurkiewicz, R. Loll
 
 The theory of causal 
	dynamical triangulations (CDT) attempts to define a nonperturbative theory 
	of quantum gravity as a sum over spacetime geometries. One of the 
	ingredients of the CDT framework is a global time foliation, which also 
	plays a central role in the quantum gravity theory recently formulated by 
	Horava. We show that the phase diagram of CDT bears a striking resemblance 
	with the generic Lifshitz phase diagram appealed to by Horava. We argue that 
	CDT might provide a unifying nonperturbative framework for anisotropic as 
	well as isotropic theories of quantum gravity.
 
 
	Dark matter as integration constant in Horava-Lifshitz gravityShinji 
	Mukohyama
 
 In the non-relativistic theory of gravitation recently 
	proposed by Horava, the Hamiltonian constraint is not a local equation 
	satisfied at each spatial point but an equation integrated over a whole 
	space. The global Hamiltonian constraint is less restrictive than its local 
	version, and allows a richer set of solutions than in general relativity. We 
	show that a component that behaves like pressureless dust emerges as an 
	integration constant of dynamical equations and momentum constraint 
	equations. So classical solutions to the infrared limit of Horava-Lifshitz 
	gravity can mimic general relativity plus cold dark matter.
 
 
	The Cosmological Constant and Horava-Lifshitz GravityCorrado Appignani, 
	Roberto Casadio, S. Shankaranarayanan
 
 Horava-Lifshitz theory of 
	gravity with detailed balance is plagued by the presence of a negative bare 
	(or geometrical) cosmological constant which makes its cosmology clash with 
	observations. We argue that adding the effects of the large vacuum energy of 
	quantum matter fields, this bare cosmological constant can be approximately 
	compensated to account for the small observed (total) cosmological constant. 
	We establish a relation between the cosmological constant and the length 
	scale of dimension 4 corrections to the Einstein gravity. We argue that 
	Lorentz invariance is broken only at very small scales.
 
 
	AR  I like it: the Lorentz 
	symmetry is philosophically procrustian in view of the arrow of time. See my 
	essay on time to reflect that the epistemologically anomalous nature of time 
	should dispose us to reserve judgment on full spacetime symmetry (chapter 13 
	in Mindworlds). Thus, too, we 
	avoid the ascent to sub specie aeternitatis fantasy of "Time Lords" 
	Einstein and Gödel (which I also gloss informally in my new book
	G.O.D. Is Great).
 
Gravity Waves 
	
	By Robin McKieThe Observer, April 15, 2012
 
	Edited by Andy Ross 
	Beside the village of Ruthe, near Hannover, Germany, scientists are hunting 
	for gravity waves. When big stars collapse into black holes or when pairs of 
	neutron stars spiral toward each other, they agitate the fabric of 
	spacetime, sending ripples of gravitational energy across the universe.
 The Ruthe laboratory is part of the joint UK-German project Geo600 to 
	measure these waves, which were predicted a century ago by Albert Einstein 
	but have not yet been detected. Once they are found and detectors become 
	more sophisticated and sensitive, astronomers will use them to peer into the 
	hearts of stars in ways that are beyond current observatories.
 
 The 
	detectors feature two long arms, set at right angles to each other, 
	extending from a lab fitted with sensitive measuring equipment. Glasgow 
	professor Jim Hough: "When a gravitational wave reaches a detector, it will 
	temporarily shrink one arm and slightly extend the other depending on its 
	angle of approach. It will be our task to measure that change."
 
 Gravitational waves are generated by enormously energetic but incredibly 
	remote events. A wave's energy is dissipated so far that the change it makes 
	in a detector is less than the diameter of a proton.
 
 This explains 
	why efforts to pinpoint gravitational waves have so far failed. But 
	scientists are confident that laser interferometry will measure them. A 
	laser beam passes through a beam splitter so that two identical beams shine 
	down each of the detector arms. At the end of each tunnel is a mirror. The 
	beams are reflected back to a detector and recombined. With careful tuning, 
	the beams can be superposed.
 
 The gravitational waves alter the 
	relative positions of the mirrors. This changes the intensity of the light 
	observed. The light waves from the beams normally arrive in phase to give a 
	bright spot. But if the mirrors move even slightly the image is darkened. 
	That is the theory.
 
 In reality, scientists have been frustrated by 
	all sorts of details. For example, if a person walks close to a mirror their 
	mass exerts a tiny gravitational influence on it, causing the mirror to 
	move. And thermal noise causes mirrors and mountings to vibrate slightly, 
	again creating spurious signals.
 
 New detectors have arms several 
	kilometers long. And great care has been taken in their construction to 
	reduce vibrations. Their arms are suspended from rails that run the length 
	of the detectors' trenches; the tubes along which the laser light is 
	channelled inside an arm contain ultra-pure vacuums; while the lasers 
	themselves are high performance industrial devices.
 
 The UK-German 
	team at Ruthe has developed delicate systems of silica mirrors and pendulums 
	use four platforms suspended from each other in layers, to isolate them from 
	vibrations, and used light squeezing to reduce quantum fluctuations in the 
	laser beam, thus easing measurement. Hough expects to see the waves by 
	around 2015.
 
 
	Where Does Spacetime Come From? 
	
	By George MusserScientific American, April 12, 2012
 
	Edited by Andy Ross 
	Two Russian physicists have proposed a new way of understanding space and 
	time. Mikhail Vasiliev and the late Efin Fradkin of the Lebedev Institute in 
	Moscow developed the theory in the late 1980s.
 The basic idea of 
	modern physics is that the world consists of fields. VF theory posits an 
	infinite number of fields. They come in progressively more complicated 
	varieties described by the quantum property of spin.
 
 Think of spin as 
	the degree of rotational symmetry. The electromagnetic field with its 
	particle, the photon, has spin 1. If you give it a full turn, it looks the 
	same as before. The gravitational field with its particle, the graviton, has 
	spin 2: you need to rotate it only half a turn. The known particles of 
	matter, such as the electron, have spin 1/2: they need 2 full turns to look 
	the same. The Higgs field has spin 0 and looks the same no matter how you 
	rotate it.
 
 In VF theory, there are also spin 5/2, spin 3, and so on, 
	all the way up. Physicists used to assume that was impossible. These 
	higher-spin fields, being more symmetrical, would imply new laws of nature 
	analogous to the conservation of energy, and no two objects could ever 
	interact without breaking one of those laws. At first glance, string theory 
	runs afoul of this principle. An elementary quantum string has an infinity 
	of higher harmonics, which correspond to higher-spin fields. But those 
	harmonics come with an energy cost, which keeps them inert.
 
 The above 
	reasoning applies only when gravity is insignificant and spacetime is not 
	curved. In curved spacetimes, higher-spin fields can exist after all.
 
 Higher-spin fields promise to flesh out the holographic principle. 
	Suppose you have a hypothetical 3D spacetime (2 space + 1 time) filled with 
	particles that interact solely by a souped-up strong nuclear force, without 
	gravity. In such a setting, objects of a given size can interact only with 
	objects of comparable size, just as objects can interact only if they are 
	spatially adjacent. Size plays exactly the same role as spatial position; 
	you can think of size as a new dimension of space. The original 3D spacetime 
	becomes the boundary of a 4D spacetime, with the new dimension representing 
	the distance from this boundary. Not only does a spatial dimension emerge, 
	but so does gravity. In the jargon, the strong nuclear force in 3D spacetime 
	(the boundary) is dual to gravity in 4D spacetime (the bulk).
 
 The 
	holographic principle describes a bulk where dark energy has negative 
	density, warping spacetime into an anti-de Sitter geometry. But dark energy 
	has positive density, to give something like a de Sitter geometry. The 
	boundary of 4D de Sitter spacetime is a 3D space lying in the infinite 
	future. The emergent dimension in this case is time. If physicists could 
	formulate a version of the holographic principle for a de Sitter geometry, 
	it would not only apply to the real universe but would also explain time.
 
 VF theory works in either an anti-de Sitter or a de Sitter geometry. In 
	the de Sitter case, the 3D boundary is governed by a static field theory. 
	The structure of this theory gives rise to time in an asymmetric way, which 
	might account for the arrow of time.
 
 In VF theory, the higher-spin 
	fields possess higher symmetry than the gravitational field, and hence less 
	structure. The general theory of relativity says spacetime is like silly 
	putty. Vasiliev theory says it is sillier putty, too silly for defining 
	consistent causal relations or keeping distant objects apart from each 
	other.
 
 VF theory is even more nonlinear than general relativity. 
	Matter and spacetime geometry are so thoroughly entwined that it becomes 
	impossible to tease them apart. The primordial universe was an amorphous 
	blob. As the higher-spin symmetries broke, spacetime emerged.
 
 The 
	Complete Idiot's Guide to String Theory
 By George Musser
 
	AR Duh. What's the next stage of dimmitude below 
	complete idiot?
 
	Quantum Gravity and LIGO 
	
	Ashutosh Jogalekar and Freeman DysonScientific American, May 3, 2013
 
	Edited by Andy Ross 
	Physicists have long dreamed of a grand unified theory embracing all known 
	forces and laws. The pioneers of thermodynamics brought together mechanics 
	and heat. Faraday and Maxwell unified electricity, magnetism, and optics. 
	Einstein unified first space and time, then matter and energy, and finally 
	spacetime and gravity in relativity theory. Unification continued with 
	wave-particle duality and with quantum field theory uniting special 
	relativity and quantum mechanics. But the union of gravity with quantum 
	theory remains intractable.
 A good way to probe quantum gravity is to 
	look for gravitons. Researchers have designed equipment so sensitive that it 
	should be able to detect a single graviton. The Laser Interferometer 
	Gravitational Wave Observatory (LIGO) uses an interferometer to detect 
	gravitational waves. A wave passing through the interferometer warps local 
	space-time and changes the effective length of one or both of the cavities. 
	This puts the light in the cavity out of phase with incoming light. The 
	cavity goes out of resonance, the beams detune, and a periodic signal will 
	emerge.
 
 But LIGO may not work. Because of ambient noise, the actual 
	LIGO detectors can only detect waves far stronger than a single graviton. 
	But even in a quiet universe, an ideal LIGO detector cannot detect a single 
	graviton. In a quiet universe, the limit to the measurement of distance is 
	set by the quantum uncertainties in the positions of the mirrors. To make 
	them small, the mirrors must be massive. To detect a single graviton with 
	LIGO hardware, the mirrors must be so massive that they attract each other 
	irresistibly and collapse into a black hole. So LIGO no go.
 
 Perhaps 
	theories of quantum gravity are untestable.
 
 >> Freeman Dyson
 
	  
		
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