A Unified Quantum Theory of the Sexual Interaction

Recent changes to the criteria for allocating research funding require particle physicists  and astronomers to justify the wider social, cultural and economic impact of their science. In view of the directive to engage in work more directly relevant to the person in the street, I’ve decided to share with you my latest results, which involve the application of ideas from theoretical physics in the wider field of human activity. That is, if you’re one of those people who likes to have sex in a field.

In the simplest theories of the sexual interaction, the eigenstates of the Hamiltonian describing all allowed forms of two-body coupling are identified with the conventional gender states, “Male” and “Female”  denoted |M> and |F> in the Dirac bra-ket notation; note that the bra is superfluous in this context so, as usual, we dispense with it at the outset. Interactions between |M> and |F> states are assumed to be attractive while those between |M> and |M> or |F> and |F> are supposed either to be repulsive or, in some theories, entirely forbidden.

Observational evidence, however, strongly  suggests that two-body interactions involving either F-F or M-M coupling, though suppressed in many  situations, are by no means ruled out  in the manner one would expect from the simplest theory outlined above. Furthermore, experiments indicate that the relevant channel for M-M interactions appears to have a comparable cross-section to that of the standard M-F variety, so a similar form of tunneling is presumably involved. This suggests that a more complete theory could be obtained by a  relatively simple modification of the  version presented above.

Inspired by the recent Nobel prize awarded for the theory of quark mixing, we are now able to present a new, unified theory of the sexual interaction. In our theory the “correct” eigenstates for sexual behaviour are not the conventional |M> and |F> gender states but linear combinations of the form

|M>=cosθ|S> + sinθ|G>

|F>=-sinθ|G>+cosθ|S>

where θ is the Cabibbo mixing angle or, more appropriately in this context, the sexual orientation (measured in degrees). Extension to three states is in principle possible (but a bit complicated) and we will not discuss this issue further.

In this theory each |M> or |F> state is regarded as a linear combination of heterosexual (straight, S)  and homosexual (gay, G) states represented by a rotation of the basis by an angle θ, exactly the same mechanism that accounts for the charge-changing weak interactions between quarks.

For a purely heterosexual state, this angle is zero, in which case we recover the simple theory outlined above. At θ=90° only the G component manifests itself; in this state only classically forbidden interactions are permitted. The general state is however, one with a value of the orientation angle somewhere between these two limits and this permits all forms of interaction, at least with some probability.

Note added in proof:  the |G> states do not appear in standard QFT but are motivated by some versions of string theory, expecially those involving G-strings.

One immediate consequence of this theory is that a “pure” gender state should be generally regarded as a quantum superposition of “straight” and “gay” states. This differs from a classical theory in that the true state can not be known with certainty; only the relative frequency of straight and gay behaviour (over a large number of interactions) can be predicted, perhaps explaining the large number of married men to be found on gaydar. The state at any given time is thus entirely determined by a sum over histories up to that moment, taking into account the appropriate action. In the Copenhagen interpretation, collapse one way or another  occurs only when a measurement is made (or when enough Carlsberg is drunk).

If there is a difference in energy of the basis states a pure |M> state can oscillate between |S> and |G> according to a time-dependent phase factor arising when the two states interfere with each other:

|M(t)>=cosθ|S>exp(-iE1t) + sinθ|G>exp(-iE2t);

(obviously we are using natural units here, so that it all looks cleverer than it actually is). This equation is the origin of the expressions  “it’s just a phase he’s going through” and “he swings both ways”. In physics parlance this means that the eigenstates of the sexual interaction do not coincide with the conventional gender types, indicating that sexual behaviour is not necessarily time-invariant for a given body.

Whether single-body phenomena (i.e. self-interactions) can provide insights into this theory  depends, as can be seen from the equation,  on the energies of the relevant states (as is also the case  in neutrino oscillations). If they are equal then there is no oscillation. However,  a detailed discussion of the role of degeneracy is beyond the scope of this analysis.

Self- interactions involving a solitary phase are generally difficult to observe,  although examples have been documented that involve short-lived but highly-excited states  accompanied by various forms of stimulated emission. Unfortunately, however, the resulting fluxes are  not often well measured. This form of interaction also appears to be the current preoccupation of string theorists.

More definitive evidence for the theory might emerge from situations involving some form of entanglement, such as in the examples of M-M and F-F coupling mentioned above.  Non-local interactions of a sexual type are possible in principle, but causality and simultaneity issues exist and most researchers consequently prefer to focus on local interactions, which are generally supposed to be more satisfactory from the point-of-view of reproducibility.

Although the theory is qualitatively successful we need more experimental data to pin down the parameters needed for a robust fit. It is not known, for example, whether the rates of M-M and F-F coupling are similar or, indeed, whether the peak intensity of these interactions, when resonance is reached, is similar to those of the standard M-F form. It is generally accepted, however, that the rate of decay from peak intensity is rather slower for processes involving |F> states than for|M> which is not so easy to model in this theory, although with a bit of renormalization we can probably explain anything.

Answers to these questions can perhaps be gleaned from observations of many-body processes  (i.e. those with N≥3),  especially if they involve a multiplicity of hardon states (i.e. collective excitations). Only these permit a full exploration of all possible degrees of freedom, although higher-order Feynman diagrams are needed to depict them and they require more complicated group theoretical techniques.  Examples like the one  shown  – representing a threesome – are not well understood, but undoubtedly contribute significantly to the bi-spectrum.

One might also speculate that in these and other highly excited states,  the sexual interaction may be described by something more like the  electroweak theory in which all forms of interaction occur in a much more symmetric fashion and at much higher rates than at lower energies. That sounds like some kind of party…

It is worth remarking that there may be finer structure than this model takes into account. For example, the |G> state is generally associated with  singlet configurations like those shown on the right. However, G-G coupling is traditionally described in terms of  “top” |t> and “bottom” |b> states, with b-t coupling the preferred mode,  leading to the possibility of doublets or even triplets. It may be even prove  necessary to introduce a further mixing angle φ of the form

|G>=cosφ |t> + sinφ |b>

so that the general state of |G>  is “versatile”. However, whether G-G interactions can be adequately described even in this extended theory is a matter for debate until the intensity of t-t and b-b  coupling is more accurately measured.

Finally, we should like to point out the difference between our model and that of the usual quark sextet, in which interacting states are described in terms of three pairs: the bottom (b) and top (t) which we have mentioned already; the strange (s) and charmed (c); and the up (u) and down (d). While it is clear that |b> and |t> do exhibit strong interactions and it appears plausible that |s> and |c> might do likewise, the sexual interaction clearly breaks the isospin symmetry between the |u> and the |d> in both M-M and M-F cases. The “up” state is definitely preferred in all forms of coupling and, indeed, the “down” has only ever been known to engage in weak interactions.

We have recently submitted an application to the Science and Technology Facilities Council for a modest sum (£754 million) to build a large-scale  UK facility  in order to carry out hands-on experimental tests of some aspects of the theory. We hope we can rely on the support of the physics community in agreeing to close down their labs and quit their jobs in order to release the funding needed to support it.

48 Responses to “A Unified Quantum Theory of the Sexual Interaction”

  1. this is hilarious! count me in :)

  2. This is brilliant. I had to reread one paragraph just to understand it! Humorology at it’s finest.

  3. Haley Gomez Says:

    You are officially my hero. Please send this in to a national paper, it needs to be read by everyone.

  4. I’ve often found you get disentanglement when an external observer interrupts the resonant excitation.

  5. We have recently submitted an application to the Science and Technology Facilities Council for a modest sum (£754 million) to build a large-scale UK facility in order to carry out hands-on experimental tests of this aspect of the theory. We hope we can rely on the support of the physics community in agreeing to close down their labs and quit their jobs in order to support it.

    As long as your impact statement is hot to trot I think you have a good chance.

  6. Oh my goodness! The concept of tunneling has taken on a whole new meaning. You are a very clever but slightly strange man, Peter :-)

    PS: The black Feynman diagram on a black background is rather invisible.

  7. telescoper Says:

    How very strange. The diagram was visible yesterday but has now disappeared. I’ll see if I can get it back.

    There. I think it has appeared now.

  8. telescoper Says:

    George,

    This may happen but I think the effect of an observer can have the opposite sign in some cases.

    Peter

  9. Bloody Brilliant !

  10. Brilliant. Brilliant. Brilliant. Just inspired.

  11. Thomas D Says:

    You would of course call it the Large Hardon Collider…

  12. telescoper Says:

    No, that would be rude.

  13. > the sexual orientation (measured in degrees).
    (Applause)

  14. You could also introduce a complex Kinsey number to account for the real and imaginary parts of one’s sex life

  15. Genius. Pure genius. :)

  16. Ann Onymous Says:

    Gives whole to new meaning to the inquiry, “What’s your ‘sine’?”.

    One omission: |T state – possibly represented as a temporal variation of {|M,|F} ?

  17. Aaron F. Says:

    :D

  18. Rob Ivison Says:

    i’m with Haley.

  19. Классная статья – спасибо!

  20. Bryn Jones Says:

    What does a negative orientation angle represent?

  21. telescoper Says:

    It doesn’t affect the diagonal terms because the cosine is an even function, so M-F coupling isn’t altered. In the other cases however, it represents a preference for anti-parallel states over parallel ones.

  22. Bryn Jones Says:

    Ummm, yes, I think I understand negative angles now.

  23. […] have pursued this, as there could be funding in it. That’s what Telescoper did, in his essay A Unified Quantum Theory of the Sexual Interaction. Warning: while this is maybe kinda sorta NSFW, it is absolutely not safe for math/physics-phobes. […]

  24. […] This post was Twitted by Berry_k – Real-url.org […]

  25. Very impressive work, thanks for making this available. It’s just a shame it was 50 days too late for submission to the ArXiV.

  26. […] Quantum Theory of What? I’ll stick my head out of the ground long enough to link to this, and to remind you that my pictures are going up here, with one more day to go in this first […]

  27. […] being a computer geek, I have never been terribly good at high-level physics or maths. This post makes me want to change my mind, where it attempts to create a unified quantum theory out of […]

  28. Genius. Pure genius. [2]
    I would love to translate it to portuguese. Would you allow me to do so?

  29. […] all physics geeks: A Unified Quantum Theory of the Sexual Interaction (via Bad Astronomy). The entire post is worth quoting; nonetheless, here is a small snippet. [A]ll […]

  30. When can we expect an illustrate primer?

  31. […] This post was Twitted by CoranStow – Real-url.org […]

  32. Absolutely frigging hilarious. Eroticism for geeks at its best.

  33. Some empirical evidence suggests that |M> states with a strong |S> component are more strongly attracted to F-F doublets than |F> states are to M-M, even though the two cases would seem a priori symmetrical. This may be due to the fact that by Noether’s theorem, such a symmetry would imply a conserved quantity, and conservatives are generally not fond of the |G> state.

  34. Well done. I’m laughing my arse off while my wife looks at me strangely.

  35. While this post was supposedly ment as a parody of QCD, it’s not quite BS at all.

    http://aetherwavetheory.blogspot.com/2008/11/aether-and-symmetry-world.html

  36. Fiziker Says:

    That was wonderful. I’ve been meaning to do something very similar with expressing sexual orientation in terms of eigenstates for a while now.

  37. […] A Unified Quantum Theory of the Sexual Interaction “Warning: while this is maybe kinda sorta NSFW, it is absolutely not safe for math/physics-phobes. This is high-level jokery about low-level topics,” says Phil Plait (=via). […]

  38. […] är spännande. Bloggen In The Dark har dock publicerat en hysteriskt kul post under namnet A Unified Quantum Theory of the Sexual Interactions (hittad via Bad Astronomy). Jag skrattade i alla fall gott över kommentarer som “the sexual […]

  39. Just Brilliant, pure genius!

    keep up the nice work

  40. A Feynman diagram as pornography!! Dick (sic) would be pleased!

  41. multiplicity of “hardon” states, hyperlinked to the Wikipedia def of the real thing… funny! I had missed it the first time around, guess I have made too many hardon jokes in my time.

  42. […] case you’re interested, the most popular post of the year was this one, with more hits than any other by an enormous factor. I realise that I could raise this […]

  43. […] P.S. If you thinking this application of mixing angle is daft, then you should read this post. […]

  44. […] And Peter Coles‘ “A Unified Quantum Theory of the Sexual Interaction”: […]

  45. This is amazing work, but I’d have liked to see at least an acknowledgement of gender diverse states (trans*/intersex/genderqueer), which are all too often omitted from the literature as if they don’t exist.

    • telescoper Says:

      Good point. This is clearly an incomplete model which is unable to account for all aspects of such interactions.

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