300 research outputs found
Portfolio Optimization under Partial Information with Expert Opinions: a Dynamic Programming Approach
This paper investigates optimal portfolio strategies in a market where the
drift is driven by an unobserved Markov chain. Information on the state of this
chain is obtained from stock prices and expert opinions in the form of signals
at random discrete time points. As in Frey et al. (2012), Int. J. Theor. Appl.
Finance, 15, No. 1, we use stochastic filtering to transform the original
problem into an optimization problem under full information where the state
variable is the filter for the Markov chain. The dynamic programming equation
for this problem is studied with viscosity-solution techniques and with
regularization arguments.Comment: 31 page
Expert Opinions and Logarithmic Utility Maximization in a Market with Gaussian Drift
This paper investigates optimal portfolio strategies in a financial market
where the drift of the stock returns is driven by an unobserved Gaussian mean
reverting process. Information on this process is obtained from observing stock
returns and expert opinions. The latter provide at discrete time points an
unbiased estimate of the current state of the drift. Nevertheless, the drift
can only be observed partially and the best estimate is given by the
conditional expectation given the available information, i.e., by the filter.
We provide the filter equations in the model with expert opinion and derive in
detail properties of the conditional variance. For an investor who maximizes
expected logarithmic utility of his portfolio, we derive the optimal strategy
explicitly in different settings for the available information. The optimal
expected utility, the value function of the control problem, depends on the
conditional variance. The bounds and asymptotic results for the conditional
variances are used to derive bounds and asymptotic properties for the value
functions. The results are illustrated with numerical examples.Comment: 21 page
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠΉ ΡΡΡΡΠΈ Π½Π° ΠΏΡΠΎΠ΄ΡΠΊΡ ΠΏΠ»Π°Π·ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΈΠ½ΡΠ΅Π·Π° Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ SI-C
Synthesis of silicon carbide is interested due to the presence of a wide range of his unique mechanical, thermal and electrical properties: superhardness, strength, thermal and corrosion resistance, radiation hardness, unique semiconductor characteristics. There is a great number of nano-SiC synthesis techniques, but the unique mentioned properties of the produced SiC cannot be generally realized due to dependence on the synthesis methods. In this connection the development of new simple and productive methods for the direct synthesis of nanodispersed high-quality silicon carbide is an important problem. The paper presents the results of the plasmodynamic synthesis and the ability to control the synthesis process and to change product characteristics by the plasma jet energy. The above method can be realized in a high-speed pulse jet of the dense Si-C. The jet is generated by a pulse (~100 ?s) high-current (~100 A) coaxial magnetoplasma accelerator with graphite electrodes. The synthesized product was analyzed by some modern techniques as X-ray diffraction. The main result of the paper is a demonstration of the capabilities plasmodynamic synthesis of nanosized cubic silicon carbide. Change of the input energy level can influence on phase composition, crystals growth and particle sizes
Investigation of room temperature multispin-assisted bulk diamond 13C hyperpolarization at low magnetic fields
In this work we investigated the time behavior of the polarization of bulk
13C nuclei in diamond above the thermal equilibrium. This nonthermal nuclear
hyperpolarization is achieved by cross relaxation between two nitrogen related
paramagnetic defect species in diamond in combination with optical pumping. The
decay of the hyperpolarization at four different magnetic fields is measured.
Furthermore, we use the comparison with conventional nuclear resonance
measurements to identify the involved distances of the nuclear spin with
respect to the defects and therefore the coupling strengths. Also, a careful
look at the linewidth of the signal give valuable information to piece together
the puzzle of the hyperpolarization mechanism
ΠΠ΅ΠΎΡ ΠΈΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ Π·ΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΡ ΡΠΊΠ°ΡΠ½ΠΎΠ²ΠΎ-Π·ΠΎΠ»ΠΎΡΠΎΡΡΠ΄Π½ΡΡ ΠΌΠ΅ΡΡΠΎΡΠΎΠΆΠ΄Π΅Π½ΠΈΠΉ ΠΠ°ΠΏΠ°Π΄Π½ΠΎΠΉ Π‘ΠΈΠ±ΠΈΡΠΈ
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° Π³Π΅ΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ Π·ΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΡ Π·ΠΎΠ»ΠΎΡΠΎ-ΡΠΊΠ°ΡΠ½ΠΎΠ²ΡΡ
ΠΌΠ΅ΡΡΠΎΡΠΎΠΆΠ΄Π΅Π½ΠΈΠΉ ΠΠ°ΠΏΠ°Π΄Π½ΠΎΠΉ Π‘ΠΈΠ±ΠΈΡΠΈ. ΠΡΡΠ²Π»Π΅Π½ΠΎ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠΈΡΠ΅ΡΠΊΠΈ Π·ΠΎΠ½Π°Π»ΡΠ½ΠΎΠ΅ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΡ
ΡΡΡΡΠΊΡΡΡ Π³Π΅ΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΡ
ΠΈΠ·ΡΡΠ΅Π½Π½ΡΠ΅ ΠΌΠ΅ΡΡΠΎΡΠΎΠΆΠ΄Π΅Π½ΠΈΡ. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ Π³ΡΡΠΏΠΏΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠΈΡΡΡΡΠΈΡ
ΡΡ ΠΈ Π΄Π΅ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠΈΡΡΡΡΠΈΡ
ΡΡ (ΠΏΠΎ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡ ΠΊ Π·ΠΎΠ»ΠΎΡΠΎΡΡΠ΄Π½ΡΠΌ ΡΠ΅Π»Π°ΠΌ) ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Π° ΡΠ΅ΡΠ½Π°Ρ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½Π°Ρ ΡΠ²ΡΠ·Ρ Π·ΠΎΠ»ΠΎΡΠ° Ρ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠΎΠΌ Ρ
Π°Π»ΡΠΊΠΎΡΠΈΠ»ΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ²-ΡΠΏΡΡΠ½ΠΈΠΊΠΎΠ², Π½Π°Π±ΠΎΡ ΠΊΠΎΡΠΎΡΡΡ
ΠΌΠΎΠΆΠ΅Ρ ΠΈΠ·ΠΌΠ΅Π½ΡΡΡΡΡ Π² Ρ
ΠΎΠ΄Π΅ ΡΠ²ΠΎΠ»ΡΡΠΈΠΈ Π³ΠΈΠ΄ΡΠΎΡΠ΅ΡΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ. ΠΠ°Π±ΠΎΡ Π΄Π΅ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠΈΡΡΡΡΠΈΡ
ΡΡ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ², Π½Π°ΠΊΠ°ΠΏΠ»ΠΈΠ²Π°ΡΡΠΈΡ
ΡΡ ΠΏΠΎ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΠΈ ΡΡΠ΄Π½ΡΡ
ΡΠ΅Π», Π² ΡΠ΅Π»ΠΎΠΌ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΡΠΉ ΠΈ Π²ΠΊΠ»ΡΡΠ°Π΅Ρ Π² ΡΠ΅Π±Ρ Ni, Co, Cr, V, Ba, Mn. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π°ΡΠΏΠ΅ΠΊΡΠΎΠ² Π²ΡΡΠ²Π»Π΅Π½Π½ΠΎΠΉ Π³Π΅ΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ Π·ΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΠΈ
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