190 research outputs found
A large time asymptotics for transparent potentials for the Novikov-Veselov equation at positive energy
In the present paper we begin studies on the large time asymptotic behavior
for solutions of the Cauchy problem for the Novikov--Veselov equation (an
analog of KdV in 2 + 1 dimensions) at positive energy. In addition, we are
focused on a family of reflectionless (transparent) potentials parameterized by
a function of two variables. In particular, we show that there are no isolated
soliton type waves in the large time asymptotics for these solutions in
contrast with well-known large time asymptotics for solutions of the KdV
equation with reflectionless initial data
Monosynaptic pathway from rat vibrissa motor cortex to facial motor neurons revealed by lentivirus-based axonal tracing
The mammalian motor cortex typically innervates motor neurons indirectly via oligosynaptic pathways. However, evolution of skilled digit movements in humans, apes, and some monkey species is associated with the emergence of abundant monosynaptic cortical projections onto spinal motor neurons innervating distal limb muscles. Rats perform skilled movements with their whiskers, and we examined the possibility that the rat vibrissa motor cortex (VMC) projects monosynaptically onto facial motor neurons controlling the whisker movements. First, single injections of lentiviruses to VMC sites identified by intracortical microstimulations were used to label a distinct subpopulation of VMC axons or presynaptic terminals by expression of enhanced green fluorescent protein (GFP) or GFP-tagged synaptophysin, respectively. Four weeks after the injections, GFP and synaptophysin-GFP labeling of axons and putative presynaptic terminals was detected in the lateral portion of the facial nucleus (FN), in close proximity to motor neurons identified morphologically and by axonal back-labeling from the whisker follicles. The VMC projections were detected bilaterally, with threefold larger density of labeling in the contralateral FN. Next, multiple VMC injections were used to label a large portion of VMC axons, resulting in overall denser but still laterally restricted FN labeling. Ultrastructural analysis of the GFP-labeled VMC axons confirmed the existence of synaptic contacts onto dendrites and somata of FN motor neurons. These findings provide anatomical demonstration of monosynaptic VMC-to-FN pathway in the rat and show that lentivirus-based expression of GFP and GFP-tagged presynaptic proteins can be used as a high-resolution neuroanatomical tracing method
Π‘ΠΈΠ½ΡΠ΅Π· ΡΠ° Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½Π° Π°ΠΊΡΠΈΠ²Π½ΡΡΡΡ ΡΡΠΈΡΡΠΎΡΠΎΠΌΠ΅ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ Π°Π½ΡΠ»ΡΠ΄ΡΠ² 4-Π³ΡΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΡΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΡΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠ½ΠΎΠ²ΠΈΡ ΠΊΠΈΡΠ»ΠΎΡ
In order to reveal the regularities of the βstructure β biological activityβ relationship by interaction of esters of 1-R-4-hydroxy-2,2-dioxo-1H-2Ξ»6,1-benzothiazin-3-carboxylic acids and trifluoromethyl substituted anilines in boiling xylene with good yields and purity the corresponding N-aryl-4-hydroxy-2,2-dioxo-1H-2Ξ»6,1-benzothiazin-3-carboxamides have been synthesized. The structure of the compounds obtained has been confirmed by the data of elemental analysis and NMR 1Hspectroscopy. It has been shown that the presence of trifluoromethyl groups having the powerful electron-withdrawing properties affects the position of signals of the aniline moiety protons: comparing to the spectra of the model methyl derivatives they undergo a significant paramagnetic shift. According to the results of the pharmacological studies conducted it has been found that the replacement of methyl groups in the anilide moiety of 1-R-4-hydroxy-2,2-dioxo-1H-2Ξ»6,1-benzothiazin-3-carboxamides to trifluoromethyl has a different effect on their analgesic activity, which can remain at the original level, be completely lost or significantly increase. However, N-aryl-4-hydroxy-2,2-dioxo-1H-2Ξ»6,1-benzothiazin-3-carboxamides definitely lose the ability to influence in any way on the excretory renal function after this chemical modification.Π‘ ΡΠ΅Π»ΡΡ Π²ΡΡΠ²Π»Π΅Π½ΠΈΡ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠ΅ΠΉ ΡΠ²ΡΠ·ΠΈ Β«ΡΡΡΡΠΊΡΡΡΠ° β Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΒ» Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΡΠ»ΠΎΠΆΠ½ΡΡ
ΡΡΠΈΡΠΎΠ² 1-R-4-Π³ΠΈΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΠΈΠΎΠΊΡΠΎ-1H-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΠΈΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠ½ΠΎΠ²ΡΡ
ΠΊΠΈΡΠ»ΠΎΡ ΠΈ ΡΡΠΈΡΡΠΎΡΠΌΠ΅ΡΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
Π°Π½ΠΈΠ»ΠΈΠ½ΠΎΠ² Π² ΠΊΠΈΠΏΡΡΠ΅ΠΌ ΠΊΡΠΈΠ»ΠΎΠ»Π΅ Ρ Ρ
ΠΎΡΠΎΡΠΈΠΌΠΈ Π²ΡΡ
ΠΎΠ΄Π°ΠΌΠΈ ΠΈ ΡΠΈΡΡΠΎΡΠΎΠΉ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½Ρ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠ΅ N-Π°ΡΠΈΠ»-4-Π³ΠΈΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΠΈΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΠΈΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΠΈΠ΄Ρ. Π‘ΡΡΠΎΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½ΠΎ Π΄Π°Π½Π½ΡΠΌΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ Π―ΠΠ 1Π. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠ΅ ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΡ
ΠΌΠΎΡΠ½ΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ°ΠΊΡΠ΅ΠΏΡΠΎΡΠ½ΡΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ ΡΡΠΈΡΡΠΎΡΠΌΠ΅ΡΠΈΠ»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ ΡΠΊΠ°Π·ΡΠ²Π°Π΅ΡΡΡ Π½Π° ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΈ ΡΠΈΠ³Π½Π°Π»ΠΎΠ² ΠΏΡΠΎΡΠΎΠ½ΠΎΠ² Π°Π½ΠΈΠ»ΠΈΠ΄Π½ΡΡ
ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠΎΠ² β ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ ΡΠΎ ΡΠΏΠ΅ΠΊΡΡΠ°ΠΌΠΈ ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΡΡ
ΠΌΠ΅ΡΠΈΠ»ΡΠ½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
ΠΎΠ½ΠΈ ΠΏΡΠ΅ΡΠ΅ΡΠΏΠ΅Π²Π°ΡΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΉ ΠΏΠ°ΡΠ°ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΉ ΡΠ΄Π²ΠΈΠ³. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΡ
ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ Π½Π°ΠΉΠ΄Π΅Π½ΠΎ, ΡΡΠΎ Π·Π°ΠΌΠ΅Π½Π° ΠΌΠ΅ΡΠΈΠ»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ Π² Π°Π½ΠΈΠ»ΠΈΠ΄Π½ΠΎΠΌ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ΅ 1-R-4-Π³ΠΈΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΠΈΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΠΈΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΠΈΠ΄ΠΎΠ² Π½Π° ΡΡΠΈΡΡΠΎΡ-ΠΌΠ΅ΡΠΈΠ»ΡΠ½ΡΠ΅ ΠΏΠΎ-ΡΠ°Π·Π½ΠΎΠΌΡ Π²Π»ΠΈΡΠ΅Ρ Π½Π° ΠΈΡ
Π°Π½Π°Π»ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ, ΠΊΠΎΡΠΎΡΠ°Ρ ΠΌΠΎΠΆΠ΅Ρ ΠΎΡΡΠ°Π²Π°ΡΡΡΡ Π½Π° ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΌ ΡΡΠΎΠ²Π½Π΅, ΠΏΠΎΠ»Π½ΠΎΡΡΡΡ ΡΠ΅ΡΡΡΡΡΡ ΠΈΠ»ΠΈ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΡΠΈΠ»ΠΈΠ²Π°ΡΡΡΡ. Π Π²ΠΎΡ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ Π²Π»ΠΈΡΡΡ ΠΊΠ°ΠΊΠΈΠΌ-Π»ΠΈΠ±ΠΎ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ Π½Π° ΠΌΠΎΡΠ΅Π²ΡΠ΄Π΅Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ ΡΡΠ½ΠΊΡΠΈΡ ΠΏΠΎΡΠ΅ΠΊ N-Π°ΡΠΈΠ»-4-Π³ΠΈΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΠΈΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΠΈΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΠΈΠ΄Ρ ΠΏΠΎΡΠ»Π΅ ΡΠΊΠ°Π·Π°Π½Π½ΠΎΠΉ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΎΠ΄Π½ΠΎΠ·Π½Π°ΡΠ½ΠΎ ΡΡΡΠ°ΡΠΈΠ²Π°ΡΡ.Π ΠΌΠ΅ΡΠΎΡ Π²ΠΈΡΠ²Π»Π΅Π½Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΡΡΠ½ΠΎΡΡΠ΅ΠΉ Π·Π²βΡΠ·ΠΊΡ Β«ΡΡΡΡΠΊΡΡΡΠ° β Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½Π° Π°ΠΊΡΠΈΠ²Π½ΡΡΡΡΒ» Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡΡ Π΅ΡΡΠ΅ΡΡΠ² 1-R-4-Π³ΡΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΡΠΎΠΊΡΠΎ-1H-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΡΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠ½ΠΎΠ²ΠΈΡ
ΠΊΠΈΡΠ»ΠΎΡ ΡΠ° ΡΡΠΈΡΡΠΎΡΠΎΠΌΠ΅ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
Π°Π½ΡΠ»ΡΠ½ΡΠ² Ρ ΠΊΠΈΠΏΠ»ΡΡΠΎΠΌΡ ΠΊΡΠΈΠ»ΠΎΠ»Ρ Π· Π΄ΠΎΠ±ΡΠΈΠΌΠΈ Π²ΠΈΡ
ΠΎΠ΄Π°ΠΌΠΈ Ρ ΡΠΈΡΡΠΎΡΠΎΡ ΡΠΈΠ½ΡΠ΅Π·ΠΎΠ²Π°Π½Ρ Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½Ρ N-Π°ΡΠΈΠ»-4-Π³ΡΠ΄ΡΠΎΠΊΡΠΈ- 2,2-Π΄ΡΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΡΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΡΠ΄ΠΈ. ΠΡΠ΄ΠΎΠ²Π° ΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ Π΄ΠΎΠ²Π΅Π΄Π΅Π½Π° Π΄Π°Π½ΠΈΠΌΠΈ Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΡΠ·Ρ ΡΠ° ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΡΡ Π―ΠΠ 1Π. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΠΎ ΠΏΡΠΈΡΡΡΠ½ΡΡΡΡ ΡΡΠΈΡΡΠΎΡΠΎΠΌΠ΅ΡΠΈΠ»ΡΠ½ΠΈΡ
Π³ΡΡΠΏ, ΡΠΊΡ Π²ΠΈΡΠ²Π»ΡΡΡΡ ΡΠΈΠ»ΡΠ½Ρ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ°ΠΊΡΠ΅ΠΏΡΠΎΡΠ½Ρ Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΡ, ΠΏΠΎΠ·Π½Π°ΡΠ°ΡΡΡΡΡ Π½Π° ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½Ρ ΡΠΈΠ³Π½Π°Π»ΡΠ² ΠΏΡΠΎΡΠΎΠ½ΡΠ² Π°Π½ΡΠ»ΡΠ΄Π½ΠΈΡ
ΡΡΠ°Π³ΠΌΠ΅Π½ΡΡΠ² β ΠΏΠΎΡΡΠ²Π½ΡΠ½ΠΎ Π·Ρ ΡΠΏΠ΅ΠΊΡΡΠ°ΠΌΠΈ ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΠΈΡ
ΠΌΠ΅ΡΠΈΠ»ΡΠ½ΠΈΡ
ΠΏΠΎΡ
ΡΠ΄Π½ΠΈΡ
Π²ΠΎΠ½ΠΈ ΠΏΡΠ΄Π΄Π°ΡΡΡΡΡ ΡΡΡΡΡΠ²ΠΎΠΌΡ ΠΏΠ°ΡΠ°ΠΌΠ°Π³Π½ΡΡΠ½ΠΎΠΌΡ Π·ΡΡΠ²Ρ. ΠΠ° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ
ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΈΡ
Π²ΠΈΠΏΡΠΎΠ±ΠΎΠ²ΡΠ²Π°Π½Ρ Π·Π½Π°ΠΉΠ΄Π΅Π½ΠΎ, ΡΠΎ Π·Π°ΠΌΡΠ½Π° ΠΌΠ΅ΡΠΈΠ»ΡΠ½ΠΈΡ
Π³ΡΡΠΏ Π² Π°Π½ΡΠ»ΡΠ΄Π½ΠΎΠΌΡ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΡ 1-R-4-Π³ΡΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΡΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΡΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΡΠ΄ΡΠ² Π½Π° ΡΡΠΈΡΡΠΎΡΠΎΠΌΠ΅ΡΠΈΠ»ΡΠ½Ρ ΠΏΠΎ-ΡΡΠ·Π½ΠΎΠΌΡ Π²ΠΏΠ»ΠΈΠ²Π°Ρ Π½Π° ΡΡ
Π°Π½Π°Π»Π³Π΅ΡΠΈΡΠ½Ρ Π°ΠΊΡΠΈΠ²Π½ΡΡΡΡ, ΡΠΊΠ° ΠΌΠΎΠΆΠ΅ Π·Π°Π»ΠΈΡΠ°ΡΠΈΡΡ Π½Π° Π²ΠΈΡ
ΡΠ΄Π½ΠΎΠΌΡ ΡΡΠ²Π½Ρ, ΠΏΠΎΠ²Π½ΡΡΡΡ Π²ΡΡΠ°ΡΠ°ΡΠΈΡΡ Π°Π±ΠΎ ΠΆ Π·Π½Π°ΡΠ½ΠΎ ΠΏΠΎΡΠΈΠ»ΡΠ²Π°ΡΠΈΡΡ. Π ΠΎΡΡ Π·Π΄Π°ΡΠ½ΡΡΡΡ Π²ΠΏΠ»ΠΈΠ²Π°ΡΠΈ Π±ΡΠ΄Ρ-ΡΠΊΠΈΠΌ ΡΠΈΠ½ΠΎΠΌ Π½Π° ΡΠ΅ΡΠΎΠ²ΠΈΠ΄ΡΠ»ΡΠ½Ρ ΡΡΠ½ΠΊΡΡΡ Π½ΠΈΡΠΎΠΊ N-Π°ΡΠΈΠ»-4-Π³ΡΠ΄ΡΠΎΠΊΡΠΈ-2,2-Π΄ΡΠΎΠΊΡΠΎ-1Π-2Ξ»6,1-Π±Π΅Π½Π·ΠΎΡΡΠ°Π·ΠΈΠ½-3-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΡΠ΄ΠΈ ΠΏΡΡΠ»Ρ Π·Π°Π·Π½Π°ΡΠ΅Π½ΠΎΡ Ρ
ΡΠΌΡΡΠ½ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ ΠΎΠ΄Π½ΠΎΠ·Π½Π°ΡΠ½ΠΎ Π²ΡΡΠ°ΡΠ°ΡΡΡ
The Gould-Hopper Polynomials in the Novikov-Veselov equation
We use the Gould-Hopper (GH) polynomials to investigate the Novikov-Veselov
(NV) equation. The root dynamics of the -flow in the NV equation is
studied using the GH polynomials and then the Lax pair is found. In particulr,
when , one can get the Gold-fish model. The smooth rational solutions
of the NV equation are also constructed via the extended Moutard transformation
and the GH polynomials. The asymptotic behavior is discussed and then the
smooth rational solution of the Liouville equation is obtained.Comment: 22 pages, no figur
Towards an Inverse Scattering theory for non decaying potentials of the heat equation
The resolvent approach is applied to the spectral analysis of the heat
equation with non decaying potentials. The special case of potentials with
spectral data obtained by a rational similarity transformation of the spectral
data of a generic decaying potential is considered. It is shown that these
potentials describe solitons superimposed by Backlund transformations to a
generic background. Dressing operators and Jost solutions are constructed by
solving a DBAR-problem explicitly in terms of the corresponding objects
associated to the original potential. Regularity conditions of the potential in
the cases N=1 and N=2 are investigated in details. The singularities of the
resolvent for the case N=1 are studied, opening the way to a correct definition
of the spectral data for a generically perturbed soliton.Comment: 22 pages, submitted to Inverse Problem
Topological Phenomena in the Real Periodic Sine-Gordon Theory
The set of real finite-gap Sine-Gordon solutions corresponding to a fixed
spectral curve consists of several connected components. A simple explicit
description of these components obtained by the authors recently is used to
study the consequences of this property. In particular this description allows
to calculate the topological charge of solutions (the averaging of the
-derivative of the potential) and to show that the averaging of other
standard conservation laws is the same for all components.Comment: LaTeX, 18 pages, 3 figure
Isoperiodic deformations of the acoustic operator and periodic solutions of the Harry Dym equation
We consider the problem of describing the possible spectra of an acoustic
operator with a periodic finite-gap density. We construct flows on the moduli
space of algebraic Riemann surfaces that preserve the periods of the
corresponding operator. By a suitable extension of the phase space, these
equations can be written with quadratic irrationalities.Comment: 15 page
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