1,146 research outputs found
ΠΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠ°Ρ ΡΠΎΡΠ³ΠΎΠ²Π»Ρ ΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ
This paper aims to examine how corporate insider trading influences trading patterns of foreign and institutional investors especially in firms with high discretionary accruals and low book-to-market ratios as proxies for information uncertainty. This study uses methods such as trading patterns of informed traders who are considered to gather more precise information before and after insider trading and tests how insider trading affects informed traders. The results of this study provide evidence that insider trading is likely to influence informed tradersβ trading patterns. After controlling for firm-specific factors, this study finds that the event and the amount of insider trading affect significantly foreign and institutional trading patterns. Furthermore, the relation between informed trading and insider trading is more enhanced when firms have a high level of discretionary accruals and a low book-to-market ratio. Prior studies have focused on the association between abnormal returns of insider trading and types of insider information disseminated, while informed trading patterns and insider trading with information uncertainty have not been specifically considered. This study enables practitioners to interpret corporate insider trading with information uncertainty on informed trading patterns.Π¦Π΅Π»ΡΡ Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°Π±ΠΎΡΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ Π½Π° ΡΠΎΡΠ³ΠΎΠ²ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΠΎΡΡΡΠ°Π½Π½ΡΡ
ΠΈ ΠΈΠ½ΡΡΠΈΡΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΠΈΠ½Π²Π΅ΡΡΠΎΡΠΎΠ², ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎ Π² ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΡΡ
Ρ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ Π΄ΠΈΡΠΊΡΠ΅ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ Π½Π°ΡΠΈΡΠ»Π΅Π½ΠΈΡΠΌΠΈ ΠΈ Π½ΠΈΠ·ΠΊΠΈΠΌ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠΌ Β«ΠΊΠ½ΠΈΠ³Π° ΠΊ ΡΡΠ½ΠΊΡΒ» Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π½Π΅ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΠΎΡΡΠΈ. Π Π΄Π°Π½Π½ΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΡΡ ΡΠ°ΠΊΠΈΠ΅ ΠΌΠ΅ΡΠΎΠ΄Ρ, ΠΊΠ°ΠΊ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠ΅ΠΉΠ΄Π΅ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅, ΠΊΠ°ΠΊ ΡΡΠΈΡΠ°Π΅ΡΡΡ, ΡΠΎΠ±ΠΈΡΠ°ΡΡ Π±ΠΎΠ»Π΅Π΅ ΡΠΎΡΠ½ΡΡ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ Π΄ΠΎ ΠΈ ΠΏΠΎΡΠ»Π΅ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ, ΠΈ ΠΏΡΠΎΠ²Π΅ΡΡΠ΅ΡΡΡ, ΠΊΠ°ΠΊ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠ°Ρ ΡΠΎΡΠ³ΠΎΠ²Π»Ρ Π²Π»ΠΈΡΠ΅Ρ Π½Π° ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠ΅ΠΉΠ΄Π΅ΡΠΎΠ². Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΡΡ ΠΎ ΡΠΎΠΌ, ΡΡΠΎ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠ°Ρ ΡΠΎΡΠ³ΠΎΠ²Π»Ρ, Π²Π΅ΡΠΎΡΡΠ½ΠΎ, Π²Π»ΠΈΡΠ΅Ρ Π½Π° ΡΠΎΡΠ³ΠΎΠ²ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠ΅ΠΉΠ΄Π΅ΡΠΎΠ². ΠΠΎΡΠ»Π΅ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΡΠ°ΠΊΡΠΎΡΠΎΠ², ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ½ΡΡ
Π΄Π»Ρ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠΉ ΡΠΈΡΠΌΡ, Π΄Π°Π½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΠ±Π½Π°ΡΡΠΆΠΈΠ»ΠΎ, ΡΡΠΎ ΡΠΎΠ±ΡΡΠΈΠ΅ ΠΈ ΠΎΠ±ΡΠ΅ΠΌ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ Π²Π»ΠΈΡΡΡ Π½Π° ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ ΠΈΠ½ΠΎΡΡΡΠ°Π½Π½ΡΡ
ΠΈ ΠΈΠ½ΡΡΠΈΡΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΡΠ΅ΠΉΠ΄Π΅ΡΠΎΠ². ΠΠΎΠ»Π΅Π΅ ΡΠΎΠ³ΠΎ, ΡΠ²ΡΠ·Ρ ΠΌΠ΅ΠΆΠ΄Ρ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»Π΅ΠΉ ΡΡΠΈΠ»ΠΈΠ²Π°Π΅ΡΡΡ, ΠΊΠΎΠ³Π΄Π° ΡΠΈΡΠΌΡ ΠΈΠΌΠ΅ΡΡ Π²ΡΡΠΎΠΊΠΈΠΉ ΡΡΠΎΠ²Π΅Π½Ρ Π΄ΠΈΡΠΊΡΠ΅ΡΠΈΠΎΠ½Π½ΡΡ
Π½Π°ΡΠΈΡΠ»Π΅Π½ΠΈΠΉ ΠΈ Π½ΠΈΠ·ΠΊΠΈΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ Β«ΠΊΠ½ΠΈΠ³Π° ΠΊ ΡΡΠ½ΠΊΡΒ». ΠΡΠ΅Π΄ΡΠ΄ΡΡΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π±ΡΠ»ΠΈ ΡΠΎΡΡΠ΅Π΄ΠΎΡΠΎΡΠ΅Π½Ρ Π½Π° ΡΠ²ΡΠ·ΠΈ ΠΌΠ΅ΠΆΠ΄Ρ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΠΎΠΉ Π΄ΠΎΡ
ΠΎΠ΄Π½ΠΎΡΡΡΡ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ ΠΈ Π²ΠΈΠ΄Π°ΠΌΠΈ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎΡ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΠΎΠ², Π² ΡΠΎ Π²ΡΠ΅ΠΌΡ ΠΊΠ°ΠΊ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ ΠΈ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π½Π΅ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΠΎΡΡΠΈ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎ Π½Π΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π»ΠΈΡΡ. ΠΠ°Π½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ°ΠΌ ΠΈΠ½ΡΠ΅ΡΠΏΡΠ΅ΡΠΈΡΠΎΠ²Π°ΡΡ ΠΊΠΎΡΠΏΠΎΡΠ°ΡΠΈΠ²Π½ΡΡ ΠΈΠ½ΡΠ°ΠΉΠ΄Π΅ΡΡΠΊΡΡ ΡΠΎΡΠ³ΠΎΠ²Π»Ρ Ρ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π½Π΅ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΠΎΡΡΡΡ Π½Π° ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠΎΡΠ³ΠΎΠ²Π»ΠΈ
Ricci Flat Black Holes and Hawking-Page Phase Transition in Gauss-Bonnet Gravity and Dilaton Gravity
It is well-known that there exists a Hawking-Page phase transition between a
spherical AdS black hole and a thermal AdS space. The phase transition does not
happen between a Ricci flat AdS black hole whose horizon is a Ricci flat space
and a thermal AdS space in the Poincare coordinates. However, the Hawking-Page
phase transition occurs between a Ricci flat AdS black hole and an AdS soliton
if at least one of horizon coordinates for the Ricci flat black hole is
compact. We show a similar phase transition betwen the Ricci flat black holes
and deformed AdS solitons in the Gauss-Bonnet gravity and the dilaton gravity
with a Liouville-type potential including the gauged supergravity coming from
the spherical reduction of Dp-branes in type II supergravity. In contrast to
Einstein gravity, we find that the high temperature phase can be dominated
either by black holes or deformed AdS solitons depending on parameters.Comment: Latex, 17 pages without figure
Schwinger Pair Production at Finite Temperature in Scalar QED
In scalar QED we study the Schwinger pair production from an initial ensemble
of charged bosons when an electric field is turned on for a finite period
together with or without a constant magnetic field. The scalar QED Hamiltonian
depends on time through the electric field, which causes the initial ensemble
of bosons to evolve out of equilibrium. Using the Liouville-von Neumann method
for the density operator and quantum states for each momentum mode, we
calculate the Schwinger pair-production rate at finite temperature, which is
the pair-production rate from the vacuum times a thermal factor of the
Bose-Einstein distribution.Comment: RevTex 10 pages, no figure; replaced by the version accepted in Phys.
Rev. D; references correcte
Nonperturbative QED Effective Action at Finite Temperature
We advance a novel method for the finite-temperature effective action for
nonequilibrium quantum fields and find the QED effective action in
time-dependent electric fields, where charged pairs evolve out of equilibrium.
The imaginary part of the effective action consists of thermal loops of the
Fermi-Dirac or Bose-Einstein distribution for the initial thermal ensemble
weighted with factors for vacuum fluctuations. And the real part of the
effective action is determined by the mean number of produced pairs, vacuum
polarization, and thermal distribution. The mean number of produced pairs is
equal to twice the imaginary part. We explicitly find the finite-temperature
effective action in a constant electric field.Comment: RevTex4, 6pages, no figure; replaced by the version to be published
in Phys. Rev.
Kajian Perancangan Karakter Maskot Universitas Pendidikan Mandalika
Mascot is a promotional media that is familiar in promotional media. Several companies to universities have mascots as icons that can represent higher education. UNDIKMA as a new joint-form campus has not used the media in the form of mascots for promotion. considering that NTB is a heterogeneous region with respect to ethnicity, religion, and race, so it requires a mascot as a brand ambassador for UNDIKMA. This is important because in the NTB region there is no tertiary institution that has a mascot. In the previous study, there was no study on mascot creation for universities. The purpose of this research is to design a mascot with a method approach that puts forward the target audience. While the method used is the Design Thinking Method developed by Tim Brown. Design thinking is a way to solve ambiguous and unfamiliar problems, rediscover problems in a human-centered way, brainstorm to generate multiple ideas, and take a hands-on approach. Very useful for prototyping and testing. Design thinking also includes continuous experimentation, such as sketching, prototyping, experimenting, and trying out different concepts and ideas. The target outcome of this research is to hopefully create a mascot design. In addition, it is also hoped that the output in the form of a mascot design guide line will also be successfully written. So that the application of the mascot can be correct and in accordance with the objectives expected by the designer
Electromagnetic fields in a 3D cavity and in a waveguide with oscillating walls
We consider classical and quantum electromagnetic fields in a
three-dimensional (3D) cavity and in a waveguide with oscillating boundaries of
the frequency . The photons created by the parametric resonance are
distributed in the wave number space around along the axis of the
oscillation. When classical waves propagate along the waveguide in the one
direction, we observe the amplification of the original waves and another wave
generation in the opposite direction by the oscillation of side walls. This can
be understood as the classical counterpart of the photon production. In the
case of two opposite walls oscillating with the same frequency but with a phase
difference, the interferences are shown to occur due to the phase difference in
the photon numbers and in the intensity of the generated waves.Comment: 8 pages revTeX including 1 eps fi
Near-Infrared Coronagraphic Observations of the T Tauri Binary System UY Aur
We present a near-infrared image of UY Aur, a 0.9" separated binary system,
using the Coronagraphic Imager with Adaptive Optics on the Subaru Telescope.
Thanks to adaptive optics, the spatial resolution of our image was ~0.1" in the
full width at half maximum of the point spread function, the highest achieved.
By comparison with previous measurements, we estimated that the orbital period
is ~1640 yrs and the total mass of the binary is ~1.73 solar mass. The observed
H-band magnitude of the secondary varies by as much as 1.3 mag within a decade,
while that of the primary is rather stable. This inconstancy may arise from
photospheric variability caused by an uneven accretion rate or from the
rotation of the secondary. We detected a half-ring shaped circumbinary disk
around the binary with a bright southwest part but a barely detectable
northeast portion. The brightness ratio is ~57. Its inner radius and
inclination are about 520 AU and 42, respectively. The disk is not uniform but
has remarkable features, including a clumpy structure along the disk,
circumstellar material inside the inner cavity, and an extended armlike
structure. The circumstellar material inside the cavity probably corresponds to
a clump or material accreting from the disk onto the binary. The armlike
structure is a part of the disk, created by the accretion from the outer region
of the disk or encounters with other stellar systems.Comment: 16 pages, 6 figures; accepted for publication in A
Spatially Resolved Molecular Hydrogen Emission in the Inner 200AU Environments of Classical T Tauri Stars
We present 2.0-2.4micron integral field spectroscopy at adaptive optics
spatial resolution (~0.''1) obtained with the Near-infrared Integral Field
Spectrograph (NIFS) at Gemini North Observatory of six Classical T Tauri stars:
T Tau, DG Tau, XZ Tau, HL Tau, RW Aur and HV Tau C. In all cases, the v=1-0
S(1) (2.12 micron) emission is detected at spatially extended distances from
the central stars. The bulk of the H_2 emission is typically not spatially
coincident with the location of continuum flux. Multiple transitions detected
in the K-band spectra show that H_2 level populations are typical of gas in
thermal equilibrium with excitation temperatures in the 1800K-2300 K range.
Three of the stars have H_2 velocity profiles that are centered at the stellar
radial velocity, and three show velocity shifts with respect to the system.
Each of the stars studied here show observed excitation temperatures, spatial
extents, and kinematics of the H_2 that are most consistent with shock excited
emission from the inner regions of the known Herbig-Haro energy flows or from
wide-angle winds encompassing the outflows rather than predominantly from UV or
X-ray stimulated emission from the central stars. The data presented in this
study highlights the sensitivity of adaptive optics-fed integral field
spectroscopy for spatially resolving emission line structures in the
environments of bright young stars.Comment: 50 pages, 13 Figures. Accepted for publication in the Astrophysical
Journal. Full Resolution paper available at:
http://www.astro.sunysb.edu/tracy/pubs/Beck07.pd
A Micro Molecular Bipolar Outflow From HL Tau
We present detailed geometry and kinematics of the inner outflow toward HL
Tau observed using Near Infrared Integral Field Spectograph (NIFS) at the
Gemini-North 8-m Observatory. We analyzed H2 2.122 um emission and [Fe II]
1.644 um line emission as well as the adjacent continuum observed at a <0".2
resolution. The H2 emission shows (1) a bubble-like geometry to the northeast
of the star, as briefly reported in the previous paper, and (2) faint emission
in the southwest counterflow, which has been revealed through careful analysis.
The emission on both sides of the star show an arc 1".0 away from the star,
exhibiting a bipolar symmetry. Different brightness and morphologies in the
northeast and southwest flows are attributed to absorption and obscuration of
the latter by a flattened envelope and a circumstellar disk. The H2 emission
shows a remarkably different morphology from the collimated jet seen in [Fe II]
emission. The positions of some features coincide with scattering continuum,
indicating that these are associated with cavities in the dusty envelope. Such
properties are similar to millimeter CO outflows, although the spatial scale of
the H2 outflow in our image (~150 AU) is strikingly smaller than the mm
outflows, which often extend over 1000-10000 AU scales. The position-velocity
diagram of the H2 and [Fe II] emission do not show any evidence for kinematic
interaction between these flows. All results described above support the
scenario that the jet is surrounded by an unseen wide-angled wind, which
interacts with the ambient gas and produce the bipolar cavity and shocked H2
emission.Comment: 13 pages, 4 figures, accepted for publication in ApJ
- β¦