De harmonia inter publicam et privatam salutem in civitate

Invocatio: Q.F.F.S.

An leges civiles obligent legislatorem?

Invocatio: I.N.J.C.

De pane supersubstantiali

Invocatio: [hepreaa].

Strödde chemiske anmärkningar, til uplysning i svenska lagfarenheten

Invocatio: M.G.H.

Praecipuae caussae collisionis legum civilium

Invocatio: I.N.J.

Sapiens Stoicorum

Invocatio: I.N.J.

De methodis quibusdam trigonometricis

Dedicatio: Magnus Jacobus Alopaeus.

Ex philosophia divina

Invocatio: I.N.J.

Oeconomisk beskrifning öfwer Åbo stad, : med wederbörandes tilstädielse, under professorens i naturkunnigheten, ... Carl Fridric Mennanders inseende, som et academiskt prof. framgifwen i Åbo den [ ] Octob. 1749. af Niclas Wasström, studiosus medicinae.

Dedicated to: Carl Gustaf Tessin, Jean Georg Lilljenberg & Johan Browallius, Algot A. Scarin & Johan Leche & Jonas Synnerberg & Joachim Schultz.

Matkailun tuhat kärjessä?

Kirjallisuusarvostelu

Quantum Tomography with Phase Space Measurements

This thesis addresses the use of covariant phase space observables in quantum tomography. Necessary and sufficient conditions for the informational completeness of covariant phase space observables are proved, and some state reconstruction formulae are derived. Different measurement schemes for measuring phase space observables are considered. Special emphasis is given to the quantum optical eight-port homodyne detection scheme and, in particular, on the effect of non-unit detector efficiencies on the measured observable. It is shown that the informational completeness of the observable does not depend on the efficiencies. As a related problem, the possibility of reconstructing the position and momentum distributions from the marginal statistics of a phase space observable is considered. It is shown that informational completeness for the phase space observable is neither necessary nor sufficient for this procedure. Two methods for determining the distributions from the marginal statistics are presented. Finally, two alternative methods for determining the state are considered. Some of their shortcomings when compared to the phase space method are discussed.

Resenyheter N:o 1 1935

kuv., 17 x 25 cm

Resenyheter N:o 2 1935

kuv., 17 x 25 cm