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Wednesday, 17 January 2018

An Epidemic in India

Prologue


A disease has spread throughout this great land of ours. To be sure, this disease is not new to us Indians. In some ways it has become part of our very national DNA. It has been with us for thousands of years. What harm then, one might ask, could such a familiar disease do to our nation and civilization if we have survived thousands of years with it?

India today is not the India of old. India today is connected both within and without. Our formerly insular society is barraged with new cultural memes everyday. We must compete globally or risk being left behind.

Many will argue that that is exactly what our "New India" is doing. But then, if we're doing everything right, why are we still on the second rung of ladder of nations? Why is our name hyphenated with Pakistan but never with China? Why are we, still, in the eyes of the world and also in fact, an "also ran"?

There is one characteristic feature which distinguishes Indians from people of the nations we most wish to compete with. Ask any Indian traveler. Even the most "nationalist" amongst them will agree with this assertion. Indians - and by "Indians", I mean the upper class, upper caste, 5% " creamy layer" of our society - are a self entitled people, who cannot be bothered to clean up after themselves, lift their own luggage or display basic courtesy towards those who do the actual cleaning and lifting. This is the disease I'm referring to. It's called entitlement. I will give one illustrative example of this phenomenon.

The Stuff Which Comes Between The Prologue and Epilogue


I was sitting in the food court of Terminal 2 of the Mumbai International Airport (CSIA), passing time, waiting for my flight's boarding time. It was hard to find a table to sit at, because most tables were dirty and littered with the leftovers of previous diners. Empty KFC boxes with chicken bones, pizza boxes with the uneaten crusts, and so on. As I sat there part me thought it would be easier to just get up and throw away all the trash than to wait for someone else to do it. But, I was preoccupied with my phone going through the latest developments on twitter.

Eventually, I noticed a scrawny man in a cleaner's uniform moving towards the tables to clean them. "Good", I thought. "Finally. Someone's going to clean up this mess". Then I noticed another man, well dressed, obviously an air traveler with a great air of superiority around him, waving his finger at the cleaner, ordering him to clean the tables. Then it hit me, that the cleaner was being ordered around by this pompous looking gentleman.

Now, there are few things which annoy me more than pompous assholes ordering someone to clean up the mess left behind by other pompous assholes. So, I got up, went to the nearest dirty table and started clearing it, chicken bones, pizza crusts and all. I figured if I couldn't change how my fellow Indians behave and how they treat others who do so much for them, the least I could do was to pitch in and give this weak, meek, tired looking man a helping hand.

Now, I realise that having described the other air traveler as a "pompous asshole", it follows that I myself must be a humble saint. Or so the reader might think. I assure you I'm no such thing. I'm very far removed from saintliness or any kind. However, I do like to think, that at the very minimum, I'm a decent human. And that as a decent human, I should do the decent thing and not stand idly by when I see someone's dignity being stepped upon.

That is, in fact, all we need. Just a little bit of decency. Just a little bit of respect for the work done day and night by the nameless millions who grow our food, drive our vehicles, bring us milk and clean our homes. It does not take a gigantic personal transformation to develop such an attitude in an individual. After all, you're not being asked to give up your cushy desk job and mow the fields, milk the cows or pick up the garbage every morning. You're not even being asked to become charitable towards the less fortunate, though it would certainly not hurt to do so. All that is being asked of you, and of me, is a little bit of decency.

Just a smile and a nod for someone cleaning the toilets in that billion dollar airport or train station. Just a thank you for the driver who picks you up and drops you off. Just the smallest gestures of appreciation of the work that each person does, which makes your modern life of comforts a possibility, the same exact way, that you would want your own work to be appreciated by your superiors.

And, yes, next time you eat in a self service area, don't wait for a cleaner to come along. Clean up after yourself. Take your tray and dump the leftovers in the bin. It's there. I assure you. You might have to look for it but it's there. It won't cost you any extra calories and you'll spread positivity around you. And if you don't find a bin then look for the nearest individual with a badge or a name tag and request them politely to install a garbage bin.

Such a change in an individual's behaviour might seem like a very minor thing. But when you take many individuals, each of whom changes by just a little bit, the system as a whole can end up undergoing a dramatic transformation. That is the sort of transformation we need to make our nation more than a "also ran". And all it takes is just the tiniest bit of change in each individual's behaviour.

Epilogue


As I walked away from the food court and towards my boarding area, I saw an old man, frail, likely suffering from arthritis and other ailments. He had been eating something and a tiny morsel - the size of a pea or less - had fallen on the shiny marble floor. There was no one watching him. He could have just let that grain of food lie on the floor and no one would have held a grudge against such an old man for not bending down for such a small piece of garbage. Nevertheless, with shaking knees and a body clearly in pain, he bent down to pick up that morsel to throw it in the garbage along with the rest of the leftovers in his hand.

As he stood up our eyes met and I smiled. He smiled back and I felt a pang of joy run through me. All is not lost, I thought to myself. We can still beat this epidemic and come out better and stronger for it.

Saturday, 13 January 2018

Theoretical Physics in India

There are many research centers and researchers in India working in hep-th (High Energy Physics, Theory), gr-qc (General Relativity/Quantum Cosmology) and quant-ph (Quantum Physics). However they are scattered all over the place and I have not been able to find a place which lists the names of places and individuals working in these fields in India. So, I figured, why not make a list! Here is my attempt at making one. It is, hopefully, a continuing work to be expanded over time. Naturally, this list reflects my own bias and is not meant to be a comprehensive list of all researchers in theoretical physics in India.





































































NameInstitutionAreas of InterestPublications
Thanu PadmanabhanIUCAA, PuneClassical General Relativity, Cosmology, Emergent Gravity, Quantum GravityINSPIRE
Romesh Kaul
IMSc Chennai, CTP DelhiBlack Hole Entropy, Loop Quantum Gravity, Knot Invariants, Mathematical Physics
INSPIRE
Golam Mortuza HossainIISER, KolkataLoop Quantum Gravity, Quantum Field Theory, Black Hole Entropy, CosmologyINSPIRE
Sushant G. GhoshCTP, DelhiBlack Holes, Classical General Relativity, Gravitational CollapseINSPIRE
Ghanshyam DateIMSc, ChennaiLoop Quantum Gravity, Gravitational Waves, High Energy Theory, INSPIRE
Arun K. PatiQIC Group, HRI, AllahabadQuantum Information, Quantum Computation, Geometric PhasesINSPIRE
Rathin AdhikariCTP, DelhiStandard Model Phenomenology, Baryogenesis, Cosmology, SupersymmetryINSPIRE
Hemwati NandanGurkul Kangri University, HaridwarQCD, Classical General Relativity, Cosmology, INSPIRE
Loganayagam R.ICTS, BengaluruString Theory, Black Holes, Quantum Field TheoryINSPIRE
Kamal Lochan PanigrahiIIT KharagpurString Theory, Quantum Gravity, High Energy TheoryINSPIRE

 

Thursday, 11 January 2018

Competitive Nationalism and (the myth of) Islamic Homogeneity

Recently the Chief Minister of Karnataka, Mr. Siddharamaiah, made the following observation on twitter regarding the recent communally motivated murders in the Dakshin Kannada (South Karnataka) district. Expressing grief as the deaths of both victims from different communities, he described the tragic incidents as the results of "competitive fanaticism" between extremists on either side

This expression, "competitive fanaticism", perfectly summarizes the favored tactic of certain elements of India's polity. The goal is too keep the embers of nationalism and religious identity burning just hot enough to maintain a state of constant dread in the general public, but not so hot that the fire gets out of hand and burns down the whole village. Of course, it is impossible to control the evolution of a system as complex as human society, no matter how resourceful any individual or group of individuals might be.

One nevers knows when the fire might burn just hot enough in one place at one time and set the whole system on flames. That is why it is important for leaders of good faith to soothe the upset nerves of people who are innocent victims of such competitive fanaticism, in addition to taking all possible steps using the state's machinery to tamp down on extremist elements of any hue.

Consider this. A Muslim from Maharashtra and a muslim from Bengal in the same room. How difficult or easy would it be for a general observer to realize that the two don't come from the same cultural backgrounds? Not difficult at all, right? Even if both have facial hair and are wearing skull caps or other items identifiable as being of Muslim origin, that won't mask the differences in speech, attitude, dietary preference, clothing habits and other cultural traits, between the two. So the obvious answer is "no, it would not be difficult at all to distinguish the different regional origins of the muslims"!

Now imagine that instead of two Muslims in that room, we have two Hindus, one from Kerala and another from Gujarat. What would be answer to the question in this case? In this case, the question would not even arise, because it is **understood** that Hindus are a not a monolithic homogenous culture and that is great diversity within the people of the subcontinent who identify themselves as being "Hindu". It should also be **understood** that Indians Muslims are also not a homogenous entity. There is as much (or as little) difference in the thinking, behavior, speech, appearance and overall cultural identify of Muslims from Karnataka and Bihar as would be found between any two Hindus from the same states.

However, the competitive fanaticism which is prevalent in today's politics is based in the fundamentally incorrect premise that Indian Muslims are a homogenous entity all sharing the exact same traits. This is, of course, a complete and malicious lie, whose purpose is to simply make the demonization of Muslims that much more convenient. After all, it is very easy to direct feelings of hate towards a single, undifferentiated entity, than to hate a vast and diverse population composed of many subcultures and tribes.

Thus in order to fight those who seek to poison social discourse and sow communal hatred, it important to do three things. First, to reach out with humility, compassion and empathy towards **all** who are affected by communal violence. Second, to take all possible legal steps to counter those who wish to spread communal propaganda and hate speech. And, third and most importantly, we must celebrate and propagate at every available opportunity the diversity of thoughts, lifestyles and cultures which exist amongst all religions, communities and regions in this vast land of India.

Sunday, 3 September 2017

Herniated Disc Exercises

Found a really nice set of five simple exercises for treating herniated or bulging discs. The exercises are:

  1. Cat-cow

  2. Bird-dog

  3. Lying prone face down with elbows tucked in under your sides

  4. Superman - with your arms either by your side, or folded behind your head, or stretched out in front

  5. Cobra or Mackenzie press-ups.


[embed]https://youtu.be/b1_uxJRpQRM[/embed]

Wednesday, 9 August 2017

Fluctuation Dissipation in Quantum Gravity

In statistical mechanics we are mostly concerned with the statistical averages of various physical quantities when the system is in equilibrium.

Fluctuation is a common phenomenon in nature. Fluctuation means how much a quantity deviates from its average value. The average value of the thermodynamic observables and the size of their fluctuation about their equilibrium values can be predicted by equilibrium statistical mechanics.

Sunday, 6 August 2017

Speeding up Wordpress

One common problem with wordpress sites is that they can seem sluggish compared to, lets say, sites built with static or single-file CMSs such as grav. There are several online tools which can help you check how fast your site is and how to optimize its performance. Two of these are pingdom and Google's pagespeed insights.

Putting my site through these two tools yields the following results:

[caption id="attachment_158" align="alignnone" width="69"] Result from tools.pingdom.com[/caption]

[caption id="attachment_159" align="alignnone" width="207"] Results from Google Pagespeed Insights.[/caption]

A more comprehensive list of online tools for testing your wordpress site speed can be found here.

Nb: The fullscreen browser images were captured using the very useful Firefox plugin Fireshot.

Monday, 17 August 2015

Spacetime Geometry as Information Geometry

In an entry to the 2013 FQXi essay contest and in an accompanying paper, Jonathan Heckman, a postdoc at Harvard, put forward a scintillating new idea - that one can derive the theory of strings and of gravity starting from nothing more but a Bayesian statistical inference model in which a collective of $N$ agents (representing by points on a $d$-dimensional grid) sample a probability distribution in order to obtain the best fits to a set of parameters $\{y_1,\ldots,y_M\}$. In investigating the statistical mechanics of such a collective, he finds that their dynamics can be described by an effective field theory, which happens to be the non-linear sigma model. Further requiring that the "judgements" of the collective be stable under perturbations implies that the dimension $d$ of the manifold in which the agents are embedded must be equal to two. Furthermore, he notes that conformal invariance of the resulting two dimensional "agent space", leads us to Einstein's theory of gravity and that the effective dynamics of the collective is described by a theory of strings.


At first glance his line of reasoning appears to be impeccable, and it is only the profound nature of his conclusions that might lead one to question whether his approach has any fatal flaws. Disregarding that possibility for the time being, let us proceed towards further interpreting this ground-breaking result.


The collective lives on a two-dimensional manifold which one can naturally identify with the worldsheet swept out by a string moving in an $M$-dimensional spacetime. Moreover, the space of parameters to which the collective performs a fit must also naturally be identified with the background geometry the string is embedded in. This leads to ask, whether it makes sense to identify the points of a spacetime geometry with statistical parameters and, if so, how can one then relate our usual geometrical notions of distance, angles, etc. to information based concepts.


Cosmological Rulers


To begin, let us switch to a simpler setting - that of our usual flat Minkowski $3+1$ dimensional spacetime, within which are embedded at random locations a set of agents which resemble the wireless routers commonly used in homes and offices. Each agent transmits a single tone at fixed time intervals indicating its presence to all the other agents in its vicinity. Each agent also listens for the tone broadcast by other agents, and by accumulating many such events performs an estimate of its distance to each of the other agents. (illustration) These agents have no scales and no way to measure distances and areas. How can a distance scale arise solely from exchanging signals between agents?


First, let us consider the situation when we do have a way to measure distances. Each agent transmits a signal, say in the form of an em wave, which propagates outwards isotropically from the location of the agent. Now, conservation of energy implies that the total flux $\Phi$ through any closed surface enclosing the agent should stay the same (illustration). In particular given two spherical surfaces $S_1$ and $S_2$ of radii $r_1$ and $r_2$ (with $ r_2 > r_1 $), the flux per unit area $I$:


$$ I(r) = \frac{\Phi}{4\pi r^2} $$


is smaller the greater the distance from the agent: $ I_2 (r_2) < I_1 (r_1) $. So, when an agent $A_1$ emits a signal containing $n$-bits, another agent $A_2$ situated a distance $r_{12}$ from the first one can receive at most:


$$ m = n \frac{a}{4 \pi r_{12}^2} $$


bits of the original signal. Here $a$ is a unit of area, which characterizes the size of the "aperture" using which an agent captures signals. Alternatively, we can state that $\mathcal{A}_2$ receives a fraction of the total flux emitted by $\mathcal{A}_1$, given by:


$$ \Phi' = \Phi \frac{a}{4 \pi r_{12}^2} $$


Since all agents are identical - emit identical signals and have apertures of the same area - $\mathcal{A}_2$ can use the value of the received flux to determine the distance from $\mathcal{A}_1$ as:


$$ r_{12} = \sqrt{ \frac{a}{4 \pi} \frac{\Phi}{\Phi'} } = \sqrt{ \frac{\Phi_0}{\Phi_{12}} } $$


where, for WTLOG (without loss of generality), we have set the area of the aperture $ a = 4\pi$. $\Phi_0 = \Phi$ is the flux emitted by .$\mathcal{A}_1$ and since we are assuming all agents are identical, this can be set to a universal value $\Phi_0$. Finally, $\Phi_{12} = \Phi'$ is the flux received by $\mathcal{A}_2$ from $\mathcal{A}_1$


Let us note that since, a priori, we do not have access to any "rulers" we can only measure ratios of distances. This, in fact, is exactly what is done in most modern cosmological observations. There is no way to determine absolute distances to stars and galaxies, without reference to some celestial objects which are used as "standard candles". We observe a given standard candle - say a type Ia supernova - in some distant galaxy and determine the amount $z$ its light is red-shifted by the time it reaches us. Using some other methods we determine the physical distance that $z$ corresponds to. In this way, we map out the large scale structure of our Universe (or at least of our local neighborhood) by comparing the spectra received from various objects with each other.


In this manner, each agent $\mathcal{A}_i$ can determine its distance to any other agent $\mathcal{A}_j$ as:


$$ r_{ij} = \sqrt{ \frac{\Phi_0}{\Phi_{ij}} } $$


And since, we are in a flat background without any dissipation it is safe to assume that $\Phi_{ij} = \Phi_{ji}$ and therefore $r_{ij} = r_{ji}$.


There are two other details. First, how does a given agent $\mathcal{A}_i$ distinguish between the flux received from two different agents $\mathcal{A}_j$ and $\mathcal{A}_k$, which lie at equal distances from $\mathcal{A}_i$? Second, even with the ability to measure distances to other agents, how does any one agent reconstruct the geometry in its neighborhood? Without some sense of direction, distances alone are not sufficient to allow an agent to distinguish between two equally distant neighbors.


The first problem can be addressed by equipping each agent with a random number generator. The procedure followed by any agent is then as follows:



  1. When its first turned on, the agent generates a random number, its unique ID, and transmits that embedded with its default signal.

  2. As it receives signals from other agents, it compares the numbers it reads from their signals with its own. If it receives a signal with a number identical to its own, it generates another random number and sets that as its new ID.

  3. This process is continued until every ID the agent receives is different from its own, for some minimum specified duration.

  4. Once this equilibrium state is reached, the agent uses the measured value of incoming fluxes to associate a distance to each one of its neighbors.

  5. In the event of an ID conflict - agent receives flux signal with ID identical to its own - the system resets and starts from step 2.


The second problem, that of being able to distinguish neighbors which are equidistant from a given agent, but not coincident, can be addressed in several ways.  One possible method is


Area and Information Density


 


 


Conclusion

Wednesday, 1 October 2014

Thermodynamics and Planetary Motion

In an earlier post, I had discussed a possible derivation of Kepler's Second Law of Planetary Motion within a quantum gravity setting. Kepler's Second Law states that for a planet in orbit around another the Sun under the influence of Newtonian gravity:
the line connecting the planet to the Sun sweeps out equal areas in equal time

The basic idea involves applying Haggard and Rovelli's result about the rate of evolution of a quantum mechanical system, according to which a system in equilibrium evolves in such a way as to pass through an equal number of states in equal time intervals. Quantum Gravity (of the Loop variety) tells us that the fundamental observable in a quantum theory of geometry is the area of a surface embedded within a given spacetime.

The area swept out by a planet during the course of its motion around the Sun is far greater than $ A \gg A_p $(the basic quantum of area, where $A_p = l_p^2$ is the Planck length). However, if classical geometry as described by (classical) general relativity arises from a more fundamental quantum theory, and consistency of any theory of quantum gravity would require this, then it is natural to assume that the macroscopic area $\delta A$ swept out of by a planet in a time $\delta t$ emerges from an ensemble of quanta of Planck areas. If one could argue that planetary motion corresponds to an "equilibrium" configuration of the gravitational field, then Haggard and Rovelli's result can be applied and we obtain Kepler's Second Law as a trivial consequence.

Saturday, 12 July 2014

Transcending Bad Sci-Fi

So I was watching "Transcendence", the latest cinematic attempt to generate public hysteria about Artificial Intelligence (AI), or more specifically about Hard AI. I stopped watching around the 42 minute mark. Johnny Depp's remarkably good portrayal of a scientist dying a slow and painful death from Polonium poisoning had kept me watching despite the utter nonsense being thrown around in the name of Sci-Fi. Then I got to the point, where one of a gang of anti-AI extremists says the following whopper:
If that thing [the AI computer armed with Johnny Depp's consciousness] connects to the internet, the first thing it will do is copy itself to every networked computer in the world and there will be no way to stop it.

Take a moment to ponder this sentence. First of all, if your script centered on an AI gone rogue, hinges on whether or not the said AI successfully copies itself to "every networked computer", then you should think of a different profession that scriptwriting. I mean, seriously? THAT'S the best AI gone rogue scenario you could come up with? Second, and more seriously, this sentence suggests that the makers of the film really didn't give a crap about actually understanding the promise and perils of strong AI. Even an AI powered scriptwriting program could have come up with dozens of fantastic script ideas centered around the theme of a strong-AI gone rogue which were not in violent conflict with our basic understanding of the subject.

The problem is with the notion that said AI, which is powered by "the most powerful quantum processors on the planet", could exist independently of the cutting-edge computing hardware on which it was originally conceived. The point is simply that of all the examples of "strong"-AI (or perhaps just I) which exist in Nature all involve some sort fleshy matter built out of neurons and neurotransmitters. I am talking about brains, of course. At least considering mammalian brains as formal working examples of biological machines that exhibit strong-Intelligence, the following observation is crucial:
The software does not have an existence independent of the hardware.

In other words the "consciousness" aspect of the behavior of these strong-I machines cannot be simulated on a computer which is less complex than the brain-matter itself. Sure, one could always (in principle) take an imprint of the consciousness in brain 'X', store it on some digital memory and at some point in the future restore the consciousness by uploading the stored data into some other brain 'Y'. However, and this is crucial, while the imprint represents the individual aspects of the brain 'X's behavior, as long as it is separated from the actual brain itself it cannot exhibit any "conscious" behavior.

Coming back to the film, if the rogue AI copies "itself" (or more properly speaking creates "imprints" of itself) onto other computers of the network, those imprints would simply be fossils of the original consciousness without the advanced hardware required to sustain the computation. In other words, the threat of an AI spreading like a global digital pandemic simply cannot be realized unless and until every networked computer is as advanced as the original hardware. Given that in the film, the original hardware is described as consisting of "the most powerful quantum processors on the planet", connecting the AI to the internet would not pose any harm as long as most of the hardware on the planet was not as sophisticated as Depp's original quantum computers.

The fact that the filmmakers were unable to grasp this fact is what leads to "Transcendence" being at best a campy sci-fi movie with more in common with "Flash Gordon" that with "Blade Runner". But don't let these deep observations stop you from enjoying the rest of the film. After all, how would the AI feel if you gave up on it halfway through the movie?

Monday, 12 May 2014

Multiverse, multiverse, where art thou?

As I understand it, the multiverse concept arises as a consequence of the standard inflationary scenario which involves one or more scalar fields "rolling down" the side of a potential hill, causing an exponential increase in the "size" of the Universe soon after the Big Bang. Now the form of the potential itself varies from place to place. Though what "place to place" means, when you are talking about the time when the geometric exoskeleton of the Universe is still in the process of formation, is quite unclear to me. And because the potential varies from "place to place", different regions of spacetime inflate at different rates and generically many such exponentially inflating volumes are generated from an original patch of spacetime. This is the origin of the concept of a multiverse.

The basic assumption behind all these scenarios is that the process of growth of geometry can be correctly modeled by the inflaton-potential scenario. And this is also the Achilles heel of the multiverse paradigm. What if the inflaton-potential scenario is only an effective description of the quantum processes which lead to the formation of geometric structure? That this is the case is clear if you have come to terms with the notion that "quantum geometry" underlies "classical geometry" and things such as metric, scalar fields and potentials arise from something more primitive. The resulting picture of spacetime is that of a fluid, which emerges from the interaction of its microscopic "atomic" constituents the same way the fluid (continuous) nature of water is the result of the interactions between many many discrete $H_2 O$ molecules.

In this picture, there are no such things as "fundamental" scalar fields. What appears to be a "fundamental" scalar field is instead an order parameter describing the collective behavior of some underlying (non-scalar) degrees of freedom. Now just as the process of condensation, where water vapor turns into water, corresponds to a phase transition, the quantum geometric picture suggests that the classical continous spacetime arises due to condensation of a gas of some sort of "atoms of geometry". Such a process should be described in the language of many-body physics in terms of a transition from one phase of geometry to another. See Sabine's blog for her take on this. Also see my previous papers which talk about such a phase transition.

Anyways, if this is indeed the real picture, then the "multiverse" is simply a consequence of taking an effective description of quantum geometry far too seriously and ignoring the fact that there is a more fundamental underlying dynamics that has to be taken into account. Of course there is no reason, a priori, for ruling out that the phase transition results in the formation of "domains", where each domain describes a slightly different classical geometry in a manner similar to the formation of domains in ferromagnetism. However, there is also no reason to why these domains would correspond to separate disconnected universes, rather than one universe divided into many regions with different geometric configurations. Whether or not these domains would correspond to the size of the observable Hubble volume today depends on the details of the underlying theory. Regardless of the details, one can see that a phase transition is a finite process in time. Once it has occurred and the new phase of geometry has emerged the resulting domains will not undergo exponential expansion because, after all, the "exponential expansion" was the phase transition itself!

In short, from this perspective the "Multiverse" is a mirage, a result of sloppy reasoning which ignores the true dynamics of geometry. There is much more to be said, but this seems enough for now!

Friday, 5 July 2013

The Measurement Problem, Part 1

The Problem


The measurement problem becomes a problem only when we neglect to specify the nature of the observer's Hilbert space. Postulates I (Systems are described by vectors in a Hilbert space) and II (Time evolution occurs via some given Hamiltonian for a particular system) are fine in that regard. These two postulates deal only with the description of a quantum system. It is the third postulate (Measurement leads to collapse of state vector to an eigenstate) where there is a problem.

A measurement is said to occur whenever one quantum system - the "observer" - described by a Hilbert space ( $ H_{O} $ ) interacts with another system described by a Hilbert space ($H_{S}$). The complete Hilbert space of the system ("observer" and the "observed") is given by:
$$ H_{O+S} = H_{O} \otimes H_{S} $$
To actually realize the dichotomy between an "internal" and "external" observer, the size of the observer's Hilbert space, given by its dimension ($dim(H_O)$), must be comparable to ($dim(H_S)$) - the dimension of the Hilbert space corresponding to the system under observation. Instead, what we generally encounter is ($dim(H_O) \gg dim(H_S)$) as is the case for, say, an apparatus with a vacuum chamber and other paraphernalia which is being used to study an atomic scale sample.

In this case the apparatus is not described by the three states ($\{\ket{ready}, \ket{up}, \ket{down}\}$), but by the larger family of states ($\{\ket{ready;\alpha}, \ket{up;\alpha}, \ket{down;\alpha}$) where ($\alpha$) parametrizes the "helper" degrees of freedom of the apparatus which are not directly involved in generating the final output, but are nevertheless present in any interaction. Examples of these d.o.f are the states of the electrons in the wiring which transmits data between the apparatus and the system.

The initial state of the complete system is of the form:
$$\ket{\psi_i} = \ket{ready;\alpha} (\mu \ket{1} + \nu \ket{0} )$$
When $ H_O$ interacts with $ H_S$ in such a way, that a measurement is said to have occurred, the final state of the composite system can be written as:
$$\ket{\psi_i} = \ket{up;\alpha} (\mu_{up} \ket{1} + \nu_{up} \ket{0}) + \ket{down;\alpha} (\mu_{down} \ket{1} + \nu_{down} \ket{0})$$
In a complete self-consistent theory, one would hope that all paradoxes regarding measurement could be resolved by understanding unitary evolution of the full Hilbert space ($H_{sum}$). This is not quite the case. Consider the case when the system being observed is a spin-1/2 object with a two dimensional Hilbert space ($H_{sys}$) a basis for which can be written as ($\{ \ket{0}; \ket{1} \} $). The Hilbert space of the observing apparatus ($H_{obs}$) is large enough to describe all the possible positions of dials, meters and probes on the apparatus. Let us assume that ($H_{obs}$) can itself be written as a tensor product:
$$H_{obs} = H_{pointer} \otimes H_{res}$$
For some poorly understood reason, when ($N_{obs} \rightarrow \infty$), an interaction between the two systems - observer and subject - causes the state of the subject to "collapse" to one of the eigenstates of the operator (or "property") of the subject being measured ($\ket{\psi_{sub}} \rightarrow \ket{\phi^i_{obs}}$).

When QM was first invented, it was understood that the measuring apparatus is a classical system requiring an infinite number of degrees of freedom for its complete description. Thus the ``collapse'' that occurs is because of something that happens at the interface of the classical measuring apparatus and the quantum system being observed. This ad-hoc separation of the classical from the quantum came to known as the "Heisenberg cut" (or "Bohr cut" depending of your reading of history). Since the quantum description of systems with even a few degrees of freedom appeared to be a great technical feat in those early days, physicists didn't have much reason to worry about systems with large ($N \gg 1$) dimension Hilbert spaces.

Mechanisms for Wavevector Collapse


To address the lack of understanding of state vector collapse in QM, and to get a grasp on the description of systems with large Hilbert spaces, first the many-worlds interpretation (MWI) and later the consistent histories or decoherence framework was constructed.

Monday, 11 February 2013

Thermal Time and Kepler's Second Law

In a fascinating recent paper (arXiv:1302.0724), Haggard and Rovelli (HR) discuss the relationship between the concept of thermal time, the Tolman-Ehrenfest effect and the rate of dynamical evolution of a system - i.e., the number of distinguishable (orthogonal) states a given system transitions through in each unit of time. The last of these is also the subject of the Margolus-Levitin theorem (arXiv:quant-ph/9710043v2) according to which the rate of dynamical evolution of a macroscopic system with fixed average energy (E), has an upper bound ($\nu_{\perp}$) given by:

\begin{equation}
\label{eqn:margolus-levitin}
\nu_{\perp} \leq \frac{2E}{h}
\end{equation}

Thursday, 31 January 2013

Some things ... cannot be learned quickly

There are some things which cannot be learned quickly,
and time, which is all we have,
must be paid heavily for their acquiring.
They are the very simplest things,
and because it takes a man’s life to know them
the little new that each man gets from life
is very costly and the only heritage he has to leave.

- Ernest Hemingway (From A. E. Hotchner, Papa Hemingway, Random House, NY, 1966)

Sunday, 27 January 2013

Elementary particles and quantum geometry

Black holes are formed due to the gravitational collapse of matter - ordinary matter, consisting of the particles and excitations of the Standard Model that we know and love. These include electrons, photons, neutrinos, quarks, mesons etc, and their respective anti-particles. General Relativity tells us that the properties of (macroscopic) black holes are universal, in that they do not depend on the precise fraction of each particle species in the initial "mixture".

A black hole formed from the collapse of a non-rotating cloud of $ n$ electrons and $ n$ positrons will be neutral, non-rotating and of mass $ 2n m_e$, where $ m_e$ is the electron mass. Let us refer to this black hole as $ bh(n,e^-; n,e^+)$ or $ bh_e$ for short. A black hole formed from the collapse of cloud of $ m$ neutrinos and $ m$ anti-neutrinos, where $ m * m_{\nu} = n * m_e$ ($ m_{\nu}$ being the mass of a neutrino). According to our labeling scheme, this black hole will be labeled as $ bh(m,\nu;m,\bar\nu)$ or $ bh_{\nu}$ for short. Both black holes have the same mass $ M = n * m_e = m * m_{\mu} $ and thus the same horizon area $ A = GM/c^2$.

... and so it begins

Welcome to my blog, gentle readers. Here you will be exposed to all manner of speculation and conjecture on my part. Those with an enhanced sensitivity to non-rigorous reasoning might occasionally experience a feeling akin to motion sickness. I urge such rigor-bound passengers to depart at the earliest exit. To the rest, welcome aboard. Happy trails!