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Lectures on String Theory

Lectures on String Theory

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– 3 –<br />

If <strong>on</strong>e tries to c<strong>on</strong>struct the quantum mechanics of relativistic strings <strong>on</strong>e finds<br />

that mathematically c<strong>on</strong>sistent theory exists if and <strong>on</strong>ly if the dimensi<strong>on</strong> of spacetime<br />

where string propagates is 26. The number 26 was named the “critical dimensi<strong>on</strong>”.<br />

On the <strong>on</strong>e hand, it was pretty remarkable and unexpected to find an example<br />

of physical theory which puts restricti<strong>on</strong>s <strong>on</strong> space-time where it is defined. On the<br />

other hand, it was certainly not clear why a theory that shared at least some qualitative<br />

features with hadr<strong>on</strong>ic physics should exist in 26 dimensi<strong>on</strong>s <strong>on</strong>ly. A subsequent<br />

discovery of QCD (Quantum Chromo Dynamics) as the most appropriate candidate<br />

to describe the theory of str<strong>on</strong>g interacti<strong>on</strong>s led to a c<strong>on</strong>siderable loss of interest to<br />

string theory.<br />

In 1974, Scherk and Schwarz came up with a proposal to completely alter the<br />

view <strong>on</strong> string theory. They suggested to c<strong>on</strong>sider the massless spin two particle<br />

absent in the hadr<strong>on</strong>ic world as the gravit<strong>on</strong> – the quantum of the gravitati<strong>on</strong>al<br />

interacti<strong>on</strong>. Indeed, this particle neatly fits the properties of the gravit<strong>on</strong> – string<br />

theory predicts that this particle interacts according to the standard laws of General<br />

Relativity. Gravitati<strong>on</strong>al interacti<strong>on</strong>s have a natural scale, called the Planck mass,<br />

which is around 10 19 GeV. This is a huge number in comparis<strong>on</strong> with characteristic<br />

energies of hadr<strong>on</strong>ic physics, 100 − 200 MeV. Thus, according to their view, string<br />

theory could provide the unifying descripti<strong>on</strong> of all the particles and matter forces,<br />

including gravity and it operates <strong>on</strong> a new fundamental scale.<br />

Even if <strong>on</strong>e accepts that quantum mechanics of relativistic strings can be defined<br />

in the unusual number 26 of the space-time dimensi<strong>on</strong>s, another problem arises. Such<br />

string does not c<strong>on</strong>tain fermi<strong>on</strong>ic degrees of freedom and it predicts the existence of<br />

a particle with the negative mass squared: m 2 < 0. Such a particle, tachy<strong>on</strong>, is a<br />

source of instability and its existence indicates that either the theory is ill-defined<br />

or it is formulated around a “wr<strong>on</strong>g” ground state, or as physicists say, around a<br />

“wr<strong>on</strong>g” vacuum. Critical dimensi<strong>on</strong>, tachy<strong>on</strong> and absence of fermi<strong>on</strong>s were the<br />

puzzling features the string theory had to face.<br />

The status of string theory changed again with the discovery of supersymmetry.<br />

All universe is made of two fundamental types of particles: bos<strong>on</strong>s and fermi<strong>on</strong>s.<br />

Fermi<strong>on</strong>s c<strong>on</strong>stitute all the matter and bos<strong>on</strong>s mediate interacti<strong>on</strong>s of the matter<br />

particles. Supersymmetry is a new type of symmetry between bos<strong>on</strong>s and fermi<strong>on</strong>s<br />

(Wess and Zumino 1974). Many physicists hope today that supersymmetry could<br />

provide an underlying principle for unificati<strong>on</strong> of all interacti<strong>on</strong>s.<br />

The first success in incorporating supersymmetry in string theory was achieved<br />

in 1971 by Ram<strong>on</strong>d, who c<strong>on</strong>structed a string analogue of the Dirac equati<strong>on</strong> (the<br />

spinning string). Shortly afterwards, Neveu and Schwarz c<strong>on</strong>structed a new bos<strong>on</strong>ic<br />

string theory. They realized that the two c<strong>on</strong>structi<strong>on</strong>s were different facets of a<br />

single theory - an interacting superstring theory c<strong>on</strong>taining Neveu and Schwarz’s

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