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ENTANGLEMENT OF GAUSSIAN STATES Gerardo Adesso

ENTANGLEMENT OF GAUSSIAN STATES Gerardo Adesso

ENTANGLEMENT OF GAUSSIAN STATES Gerardo Adesso

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Introduction<br />

About eighty years after their inception, quantum mechanics and quantum theory<br />

are still an endless source of new and precious knowledge on the physical world<br />

and at the same time keep evolving in their mathematical structures, conceptual<br />

foundations, and intellectual and cultural implications. This is one of the reasons<br />

why quantum physics is still so specially fascinating to all those that approach it<br />

for the first time and never ceases to be so for those that are professionally involved<br />

with it. In particular, since the early nineties of the last century and in the last<br />

ten-fifteen years, a quiet revolution has taken place in the quantum arena. This<br />

revolution has progressively indicated and clarified that aspects once thought to be<br />

problematic, such as quantum non-separability and “spooky” actions at a distance,<br />

are actually not only the origin of paradoxes but rather some of the key ingredients<br />

that are allowing a deeper understanding of quantum mechanics, its applications<br />

to new and exciting fields of research (such as quantum information and quantum<br />

computation), and tremendous progress in the development of its mathematical and<br />

conceptual foundations. Among the key elements of the current re-foundation of<br />

quantum theory, entanglement certainly plays a very important role, also because it<br />

is a concept that can be mathematically qualified and quantified in a way that allows<br />

it to provide new and general characterizations of quantum properties, operations,<br />

and states.<br />

The existence of entangled states, stemming directly from the superposition<br />

principle, can be regarded as a founding feature, or better “the characteristic trait”<br />

(according to Schrödinger) of quantum mechanics itself. Entanglement arises when<br />

the state of two or more subsystems of a compound quantum system cannot be<br />

factorized into pure local states of the subsystems. The subsystems thus share<br />

quantum correlations which can be stronger than any classical correlation. Quantum<br />

information science was born upon the key observation that the exploitation<br />

of such nonclassical correlations enables encoding, processing and distribution of<br />

information in ways impossible, or very inefficient, with classical means. Hence<br />

the possibility of implementing entangled resources resulted in futuristic proposals<br />

(quantum teleportation, quantum cryptography, quantum computation, ...) which<br />

are now made, to a certain extent, into reality. On a broader perspective, it is now<br />

recognized that entanglement plays a fundamental role in the physics of many-body<br />

systems, in particular in critical phenomena like quantum phase transitions, and in<br />

the description of the interactions between complex systems at the quantum scale.<br />

Despite its prominent role in the physics of microscopic but also macroscopic<br />

systems, it still stands as an open issue to achieve a conclusive characterization<br />

and quantification of bipartite entanglement for mixed states, and especially to<br />

provide a definition and interpretation of multipartite entanglement both for pure<br />

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