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String theory does not say explicitly that gravity has to be connected with the quantum world, which is why Hawking discovered this in 1974. String theory is a theory of quantum mechanics that was formulated in the context of relativistic particle physics in the late 1950s by Sheldon Glashow, Steven Weinberg and Abdus Salam at the Imperial College in London. These theorists showed that the particle states of the theory could be understood as different vibrational modes of a single string stretched in a direction of spacetime. They also suggested that this string could be a fundamental particle of physics: a string is a one-dimensional object, and, because it is infinite, it has no volume, no extension in space and no size. This is an entirely different way of thinking from the usual conception of elementary particles as quantum manifestations of matter in three-dimensional space.
The theory was also falsifiable, which is why string theory was considered an interesting line of research in the mid-1970s. As it turns out, the set of string theories encompasses nearly a hundred different theories, some of which have very different properties than the others. If string theory is actually on the right track, however, then the theoretical explanation of gravity would be something that all of the different versions of string theory have in common. Because of the theory of gravity, the quantum fluctuations in spacetime would be precisely those needed to produce the observed spacetime curvature.
The technique used in that analysis showed that the string theory does have the required vibrational properties, and this was the beginning of the boom in string theory research. A few years later, string theory made a new discovery that completely revitalized the field. String theory became a new direction in the pursuit of a theory of quantum gravity, and eventually a new generation of physicists saw the possibility of using string theory to make the first steps in constructing a theory of quantum gravity.
The application of local position independence to quantum spacetime theory leads to the question of what physical properties we shall assign to the spacetime regions. We shall have to use the physics of gravity to answer that question. If a region of the spacetime world is filled with matter, then its fabric will be curved, and in relativity this curvature is proportional to its mass. Mass, in turn, is proportional to the energy of the thing making up the mass.
If spacetime is empty, then there is no mass and no gravitational interaction. The equations we get from local position independence will describe gravity as a fundamental interaction that controls all the other forces. The other forces are held in check because the objects that are governed by the forces carry stress and strain that modifies the curvature of spacetime.
The local position independence principle imposes a restriction on the form of the equations of local position independence, which determine the shape of spacetime. We can easily find an equation in the local position independence principle that gives us back a familiar equation of gravity in Einstein’s general relativity, namely, the Einstein field equations, which, written symbolically, are
That sounds a lot like our everyday world. Besides gravity, everything on Earth feels the pull of an invisible force called the weak force. A component of the weak force is the electromagnetic force, which is responsible for the glowing white-hot mass of the sun, so the makeup of the atom is not unlike the makeup of the universe: There’s dark matter, dark energy and a glowy sun at its center. But the sun is much, much bigger, and so you would expect the mass of the universe to be much less than the mass of the sun. It turns out that the mass of the universe is about the same as the mass of the sun.
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