Teori Kaluza–Klein
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Dalam Fisika, teori Kaluza-Klein (teori KK) adalah sebuah model yang berusaha mencari solusi bagi penyatuan dua gaya fundamental yaitu gaya gravitasi dan gaya elektromagnetisme. Teori ini pertama kali diumumkan pada tahun 1921 yang diusulkan oleh matematikawan Theodor Kaluza yang memperluas teori relativitas umum hingga dimensi-5 ruang-waktu. Persamaan yang dihasilkan dapat diuraikan lebih lanjut menjadi seperangkat persamaan, satu kelompok ekuivalen dengan persamaan medan Einstein, himpunan persamaan lainnya ekuivalen dengan persamaan Maxwell dan bagian terakhir mengandung suatu medan skalar ekstra yang disebut sebagai "radion".
Tinjauan
Ruang
M ×
C dikompaktifikasi atas himpunan kompak
C, dan sesudah dekomposisi Kaluza–Klein diperoleh sebuah teori medan efektif
effective field theory atas M.
Penguraian ruangwaktu 5 dimensional
five-dimensional spacetime menjadi persamaan Einstein
Einstein equations dan persamaan Maxwell empat dimensi pertama kali ditemukan oleh
Gunnar Nordström di 1914, dalam konteks teori beliau tentang gravitasi, namun selanjutnya teori tersebut dilupakan. Kaluza menerbitkan penurunannya pada 1921 sebagai sebuah upaya untuk menyatukan elektromagnetisme dengan relativitas Einstein.
Pada tahun 1926,
Oskar Klein mengusulkan bahwa dimensi ruang spasial yang ke empat sejatinya mengkeriting dalam lingkaran yang jejarinya sangat kecil, sehingga sebuah partikel yang bergerak dalam jarak yang pendek sepanjang sumbu itu akan kembali di titik mana ia berangkat. Jarak tempuh partikel hingga kembali ke tempat semula ini dikatakan sebagai ukuran dari dimensi. Dimensi ekstra ini sebuah himpunan kompak, dan fenomena ruang-waktu dengan dimensi kompak ini disebut sebagai kompaktifikasi.
Dalam geometri modern, dimensi ekstra ke 5 ini dapat difahami sebagai sebuah grup lingkaran U(1)(
circle group U(1)), sebagaimana elektromagnetisme (
electromagnetism) dapat secara esensial diformulasikan sebagai sebuah teori gauge (
gauge theory) pada sebuah fiberbundel (
fiber bundle,
circle bundle, )dengan
gauge group
U(1). Dalam teori Kaluza–Klein grup ini menyarankan bahwa simetri gauge adalah simetri dimensi kompak sirkuler. Sekali interpretasi geometris ini difahami, relatif langsung untuk menggantikan
U(1) oleh sebuah grup Lie umum (
Lie group). Perumuman demikian sering juga disebut sebagai teori Yang-Mills
(Yang–Mills theories).
Jika sebuah pembedaan ditarik, maka teori Yang-Mills berlaku di ruang-waktu datar, sedangkan Kaluza-Klein berlaku di kasus lebih umum ruang-waktu lengkung. Ruang basis teori Kaluza-Klein tidak harus ruang-waktu 4 dimensional, dapat juga sebarang manifold (pseudo-)Riemannian, atau bahkan manifold supersimetrik atau orbifold atau bahkan ruang nonkomutatif.
Sebagai sebuah pendekatan bagi teori yang menyatukan gaya-gaya fundamental alam, adalah langsung untuk menerapkan teori Kaluza-Klein dalam usaha menyatukan gravitasi dengan gaya kuat dan elektroweak dengan menggunakan grup simetri model standar (
Standard Model),
SU(3) ×
SU(2) ×
U(1).
Meskipun demikian, sebuah usaha untuk mengkonversi konstruksi geometrik menarik ini menjadi sebuah model yang bonafid bagi realitas bertungkus lumus dengan sejumlah persoalan, termasuk kenyataan bahwa
fermions harus diperkenalkan dalam suatu cara yang dibuat-buat (dalam sebuah model nonsupersimetrik). Meskipun demikian, KK, tetaplah suatu batu uji penting dalam fisika teoretik dan sering ditanamkan dalam teori yang lebih sempurna. Teori ini dikaji secara tersendiri sebagai sebuah objek geometri yang menarik dalam teori K
(K-theory).
Bahkan dengan absennya kerangka fisika teoretis yang memuaskan, ide untuk mengeksplorasi dimensi ekstra yang terkompaktifikasi tetap menarik perhatian di kalangan komunitas astrofisikawan dan fisikawan eksperimental. Berbagai ramalan, dengan konsekuensi eksperimental real dapat dibuat (dalam kasus
large extra dimensions/
warped models). Sebagai contoh, dengan prinsip paling sederhana, dapat diharapkan diperoleh gelombang berdiri
(standing waves) dalam dimensi ekstra terkompaktifikasi. Jika sebuah dimensi ekstra spasial berjari-jari
R, massa invarian (
mass) gelombang berdiri tersebut adalah
Mn =
nh/
Rc dengan
n suatu bilangan bulat (
integer),
h konstanta Planck (
Planck's constant) dan
c laju kecepatan cahaya
(speed of light). Sehimpunan massa yang mungkin ini sering disebut sebagai
Kaluza–Klein tower. Begitu juga dalam Similarly,
Teori medan kuantum termal kompaktifikasi dimensi waktu euklidean mengarah kepada
frekuensi Matsubara sehingga menghasilkan spektrum energi termal terdiskritkan.
Contoh pencaharian eksperimental termasuk usaha yang dilakukan kolaborasi
CDF , yang telah menganalisis kembali data
penumbuk partikel untuk mencari jejak efek yang terkait dengan dimensi ekstra luas/
warped models.
Brandenberger dan Vafa telah berspekulasi bahwa pada masa alam semesta dini,
inflasi kosmik
menyebabkan tiga dimensi ruang mengembang ke ukuran kosmologis di mana dimensi ruang sisa lainnya tetap mikroskopik.
Space-time-matter theory
One particular variant of Kaluza–Klein theory is
space-time-matter theory or
induced matter theory, chiefly promulgated by
Paul Wesson and other members of the so-called Space-Time-Matter Consortium.
[1] In this version of the theory, it is noted that solutions to the equation

with
RAB the five-dimensional
Ricci curvature, may be re-expressed so that in four dimensions, these solutions satisfy
Einstein's equations

with the precise form of the
Tμν following from the
Ricci-flat condition on the five-dimensional space. Since the
energy–momentum tensor Tμν
is normally understood to be due to concentrations of matter in
four-dimensional space, the above result is interpreted as saying that
four-dimensional matter is induced from geometry in five-dimensional
space.
In particular, the
soliton solutions of
RAB = 0 can be shown to contain the
Friedmann–Lemaitre–Robertson–Walker metric
in both radiation-dominated (early universe) and matter-dominated
(later universe) forms. The general equations can be shown to be
sufficiently consistent with classical
tests of general relativity to be acceptable on physical principles, while still leaving considerable freedom to also provide interesting
cosmological models.
Geometric interpretation
The Kaluza–Klein theory is striking because it has a particularly
elegant presentation in terms of geometry. In a certain sense, it looks
just like ordinary gravity in
free space, except that it is phrased in five dimensions instead of four.
The Einstein equations
The equations governing ordinary gravity in free space can be obtained from an
action, by applying the
variational principle to a certain
action. Let
M be a (
pseudo-)
Riemannian manifold, which may be taken as the
spacetime of
general relativity. If
g is the
metric on this manifold, one defines the
action S(
g) as

where
R(
g) is the
scalar curvature and vol(
g) is the
volume element. By applying the
variational principle to the action

one obtains precisely the
Einstein equations for free space:

Here,
Rij is the
Ricci tensor.
The Maxwell equations
By contrast, the
Maxwell equations describing
electromagnetism can be understood to be the
Hodge equations of a
principal U(1)-bundle or
circle bundle π:
P →
M with fiber
U(1). That is, the
electromagnetic field F is a
harmonic 2-form in the space Ω
2(
M) of differentiable
2-forms on the manifold
M. In the absence of charges and currents, the free-field Maxwell equations are
- dF = 0 and d*F = 0.
where * is the
Hodge star.
The Kaluza–Klein geometry
To build the Kaluza–Klein theory, one picks an invariant metric on the circle
S1 that is the fiber of the U(1)-bundle of electromagnetism. In this discussion, an
invariant metric
is simply one that is invariant under rotations of the circle. Suppose
this metric gives the circle a total length of Λ. One then considers
metrics

on the bundle
P that are consistent with both the fiber metric, and the metric on the underlying manifold
M. The consistency conditions are:
- The projection of
to the vertical subspace
needs to agree with metric on the fiber over a point in the manifold M.
The Kaluza–Klein action for such a metric is given by

The scalar curvature, written in components, then expands to

where π* is the
pullback of the fiber bundle projection π:
P →
M. The connection
A on the fiber bundle is related to the electromagnetic field strength as

That there always exists such a connection, even for fiber bundles of arbitrarily complex topology, is a result from
homology and specifically,
K-theory. Applying
Fubini's theorem and integrating on the fiber, one gets

Varying the action with respect to the component
A, one regains the Maxwell equations. Applying the variational principle to the base metric
g, one gets the Einstein equations

with the
stress–energy tensor being given by

sometimes called the
Maxwell stress tensor.
The original theory identifies Λ with the fiber metric
g55,
and allows Λ to vary from fiber to fiber. In this case, the coupling
between gravity and the electromagnetic field is not constant, but has
its own dynamical field, the
radion.
Generalizations
In the above, the size of the loop Λ acts as a coupling constant
between the gravitational field and the electromagnetic field. If the
base manifold is four-dimensional, the Kaluza–Klein manifold
P is five-dimensional. The fifth dimension is a
compact space, and is called the
compact dimension. The technique of introducing compact dimensions to obtain a higher-dimensional manifold is referred to as
compactification.
Compactification does not produce group actions on chiral fermions
except in very specific cases: the dimension of the total space must be 2
mod 8 and the G-index of the Dirac operator of the compact space must
be nonzero.
[2]
The above development generalizes in a more-or-less straightforward fashion to general
principal G-bundles for some arbitrary
Lie group G taking the place of
U(1). In such a case, the theory is often referred to as a
Yang–Mills theory, and is sometimes taken to be synonymous. If the underlying manifold is
supersymmetric, the resulting theory is a super-symmetric Yang–Mills theory.
Empirical tests
Up to now, no experimental or observational signs of extra dimensions
have been officially reported. Many theoretical search techniques for
detecting Kaluza–Klein resonances have been proposed using the mass
couplings of such resonances with the
top quark, however until the
Large Hadron Collider
(LHC) reaches full operational power observation of such resonances are
unlikely. An analysis of results from the LHC in December 2010 severely
constrains theories with
large extra dimensions.
[3]
The observation of a
Higgs-like
boson at the LHC puts a brand new empirical test in the search for
Kaluza–Klein resonances and supersymmetric particles. The loop
Feynman diagrams
that exist in the Higgs Interactions allow any particle with electric
charge and mass to run in such a loop. Standard Model particles besides
the
top quark and
W boson
do not make big contributions to the cross-section observed in the H →
γγ decay, but if there are new particles beyond the Standard Model, they
could potentially change the ratio of the predicted Standard Model H →
γγ cross-section to the experimentally observed cross-section. Hence a
measurement of any dramatic change to the H → γγ cross section predicted
by the Standard Model is crucial in probing the physics beyond it.
Notes
- 5Dstm.org
- L. Castellani et al., Supergravity and superstrings, Vol 2, chapter V.11
- CMS Collaboration, "Search for Microscopic Black Hole Signatures at the Large Hadron Collider", http://arxiv.org/abs/1012.3375
References
- Nordström, Gunnar (1914). "Über die Möglichkeit, das elektromagnetische Feld und das Gravitationsfeld zu vereinigen". Physikalische Zeitschrift 15: 504–506. OCLC 1762351.
- Kaluza, Theodor (1921). "Zum Unitätsproblem in der Physik". Sitzungsber. Preuss. Akad. Wiss. Berlin. (Math. Phys.): 966–972. http://archive.org/details/sitzungsberichte1921preussi
- Klein, Oskar (1926). "Quantentheorie und fünfdimensionale Relativitätstheorie". Zeitschrift für Physik A 37 (12): 895–906. Bibcode:1926ZPhy...37..895K. doi:10.1007/BF01397481.
- Witten, Edward (1981). "Search for a realistic Kaluza–Klein theory". Nuclear Physics B 186 (3): 412–428. Bibcode:1981NuPhB.186..412W. doi:10.1016/0550-3213(81)90021-3.
- Appelquist, Thomas; Chodos, Alan; Freund, Peter G. O. (1987). Modern Kaluza–Klein Theories. Menlo Park, Cal.: Addison–Wesley. ISBN 0-201-09829-6. (Includes reprints of the above articles as well as those of other important papers relating to Kaluza–Klein theory.)
- Brandenberger, Robert; Vafa, Cumrun (1989). "Superstrings in the early universe". Nuclear Physics B 316 (2): 391–410. Bibcode:1989NuPhB.316..391B. doi:10.1016/0550-3213(89)90037-0.
- Duff, M. J. (1994). "Kaluza–Klein Theory in Perspective". In Lindström, Ulf (ed.). Proceedings of the Symposium ‘The Oskar Klein Centenary’. Singapore: World Scientific. pp. 22–35. ISBN 981-02-2332-3.
- Overduin, J. M.; Wesson, P. S. (1997). "Kaluza–Klein Gravity". Physics Reports 283 (5): 303–378. arXiv:gr-qc/9805018. Bibcode:1997PhR...283..303O. doi:10.1016/S0370-1573(96)00046-4.
- Wesson, Paul S. (1999). Space-Time-Matter, Modern Kaluza-Klein Theory. Singapore: World Scientific. ISBN 981-02-3588-7.
- Wesson, Paul S. (2006). Five-Dimensional Physics: Classical and Quantum Consequences of Kaluza-Klein Cosmology. Singapore: World Scientific. ISBN 981-256-661-9.
Further reading
- Grøn, Øyvind; Hervik, Sigbjørn (2007). Einstein's General Theory of Relativity. New York: Springer. ISBN 978-0-387-69199-2.
- Kaku, Michio and Robert O'Keefe. Hyperspace: A Scientific Odyssey Through Parallel Universes, Time Warps, and the Tenth Dimension. New York: Oxford University Press, 1994. ISBN 0-19-286189-1
- The CDF Collaboration, Search for Extra Dimensions using Missing Energy at CDF, (2004) (A simplified presentation of the search made for extra dimensions at the Collider Detector at Fermilab (CDF) particle physics facility.)
- John M. Pierre, SUPERSTRINGS! Extra Dimensions, (2003).
- TeV scale gravity, mirror universe, and ... dinosaurs Article from Acta Physica Polonica B by Z.K. Silagadze.
- Chris Pope, Lectures on Kaluza–Klein Theory.
- Edward Witten (2014). "A Note On Einstein, Bergmann, and the Fifth Dimension", arXiv:1401.8048; pdf