Fast polarization mechanisms in the uniaxial tungsten-bronze relaxor strontium barium niobate SBN-81.

The high-frequency dielectric response of the uniaxial strontium barium niobate crystals with 81% of Sr has been studied from 1 kHz to 30 THz along the polar c axis by means of several techniques (far infrared, time domain terahertz, high-frequency and low-frequency dielectric spectroscopies) in a wide temperature interval 20-600 K. Relaxor properties were observed in the complex dielectric response and four main excitations were ascertained below the phonon frequencies. These fast polarization mechanisms take place at THz, GHz and MHz ranges and show different temperature evolution. The central mode excitation in the THz range, related to anharmonic dynamics of cations, slightly softens from high temperatures and then hardens below T ~ 400 K. Below the phase transition (at T ~ 330 K) an additional microwave excitation appears near 10 GHz related to micro domain wall oscillations. The strongest relaxation appears in the GHz range and slows down on cooling according to the Arrhenius law. Finally, another relaxation, present in the MHz range at high temperatures, also slows down on cooling at least to the kHz range. These two relaxations are due to polar fluctuations and nanodomains dynamics. Altogether, the four excitations explain the dielectric permittivity maximum in the kHz range.

Spectroscopic studies of the ferroelectric and magnetic phase transitions in multiferroic Sr1-xBaxMnO3.

Dielectric response of perovskite Sr1-xBaxMnO3 (x = 0.43 and 0.45) ceramics was investigated using microwave, THz and infrared spectroscopic techniques in order to study the ferroelectric and antiferromagnetic phase transitions with critical temperatures TC ≈ 350 K and TN ≈ 200 K, respectively. The two lowest-frequency polar phonons are overdamped above TN and they exhibit pronounced softening on heating towards TC. Nevertheless, permittivity ε' in the THz range shows only a small anomaly at TC because the phonon contribution to ε' is rather small. The phonons are coupled with a central mode which provides the main contribution to the dielectric anomaly at TC. Thus, the ferroelectric phase transition has characteristics of a crossover from displacive to order-disorder type. At the same time, the intrinsic THz central peak is partially screened by conductivity and related Maxwell-Wagner relaxation, which dominates the microwave and lower-frequency spectra. Below TN, the ferroelectric distortion markedly decreases, which has an influence on the frequencies of both the central and soft modes. Therefore, ε' in the THz range increases at TN on cooling. In spite of the strong spin-phonon coupling near TN, surprisingly no magnetodielectric effect was observed in the THz spectra upon applying magnetic field of up to 7 T, which is in contradiction with the theoretically expected huge magnetoelectric coupling. We explain this fact as due to the insensitivity of TN to magnetic field.

Dynamics of nanoscale polarization fluctuations in a uniaxial relaxor.

We have studied neutron diffuse scattering in a Sr(0.61)Ba(0.39)Nb(2)O(6) single crystal by neutron backscattering at sub-µeV energy resolution. We can identify two response components with transverse polarization: an elastic (resolution limited) central peak, which monotonically increases with decreasing temperature, and a quasielastic central peak, having a maximum intensity around the ferroelectric phase transition close to 350 K. In contrast to previous neutron experiments on this and other relaxor materials, we were able to observe a temperature dependence of the characteristic frequency of these fluctuations, obeying the same Vogel-Fulcher law as the dynamic part of the dielectric permittivity of this material. In this way our findings provide a first direct link between the Vogel-Fulcher-type frequency dependence of dielectric permittivity and dynamic nanoscale lattice modulations with a transverse correlation length of about 5-10 unit cells.

An x-ray scattering study of Sn2P2S6: absence of incommensurate phase up to 1 GPa.

The ferroelectric phase transition in a semiconductor Sn(2)P(2)S(6) single crystal has been studied by means of high-resolution synchrotron x-ray diffraction in the pressure-temperature range where an incommensurate modulated phase has been anticipated for many years. In contrast with the predictions, the present measurements reveal only a direct ferroelectric-paraelectric phase transition close to T = 100 K, p = 1.1 GPa. In the vicinity of this phase transition, a characteristic critical diffuse scattering was observed, but no satellite peaks could be resolved there. It is concluded that the earlier hypothesis about the presence of an incommensurate phase and associated Lifshitz point in the temperature-pressure phase diagram of Sn(2)P(2)S(6) is incorrect.

The temperature dependence of the phononic band gap of NaI.

The position and size of the energy gap in the phonon density of states of NaI single crystal have been investigated by inelastic neutron scattering in a wide range of temperatures from 10 to 700 K. The results reveal a pronounced temperature effect which effectively leads to closure of the phonon gap at temperatures in the range of 700-800 K. The results are discussed in the context of studies of possible intrinsic localized modes in the phonon gap of alkali halides.

Broad-band conductivity and dielectric spectroscopy of composites of multiwalled carbon nanotubes and poly(ethylene terephthalate) around their low percolation threshold.

Composites of multiwalled carbon nanotubes with poly(ethylene terephthalate) (PET-MWCNT) with up to 3 vol% MWCNTs were prepared and characterized by broad-band AC conductivity and dielectric spectroscopy up to the infrared range using several techniques. A very low electrical percolation threshold of 0.07 vol% MWCNTs was revealed from the low-frequency conductivity plateau as well as from DC conductivity, whose values show the same critical power dependence on MWCNT concentration with the exponent t = 4.3. Above the plateau, the AC conductivity increases with frequency up to the THz range, where it becomes overlapped with the absorption of vibrational modes. The temperature dependence down to ~5 K has shown semiconductor behaviour with a concentration-independent but weakly temperature-dependent small activation energy of ~3 meV. The behaviour is compatible with the previously suggested fluctuation-induced tunnelling conductivity model through a thin (~1 nm) polymer contact layer among the adjacent MWCNTs within percolated clusters. At higher frequencies, deviations from the simple universal conductivity behaviour are observed, indicating some distribution of energy barriers for an electron hopping mechanism.

Dielectric, magnetic and structural properties of novel multiferroic Eu(0.5)Ba(0.5)TiO(3) ceramics.

Dielectric properties of Eu(0.5)Ba(0.5)TiO(3) ceramics were investigated between 10 and 300 K in the frequency range of 1 MHz-100 THz. Permittivity exhibits a strong peak near the ferroelectric phase transition at 215 K. This is mainly due to softening of the lowest frequency polar phonon revealed in THz and infrared spectra. Dielectric relaxation was observed also below the ferroelectric soft mode frequency in the whole investigated temperature region, but it is probably caused by some defects such as Eu(3 + ) cations or oxygen vacancies. This implies that the ferroelectric phase transition has predominantly a displacive character. Raman scattering spectra revealed a lowering of crystal symmetry in the ferroelectric phase and XRD analysis indicated orthorhombic A2mm symmetry below 215 K. The magnetic measurements performed at various frequencies in the field cooled and field heating regime after cooling in zero magnetic fields excluded spin glass behavior and proved an antiferromagnetic order below 1.9 K in Eu(0.5)Ba(0.5)TiO(3).

Bulk dielectric and magnetic properties of PFW-PZT ceramics: absence of magnetically switched-off polarization.

We investigated ceramics samples of solid solutions of [PbFe(2/3)W(1/3)O(3)](x)-[PbZr(0.53)Ti(0.47)O(3)](1 - x) (PFW(x)-PZT(1 - x), x = 0.2 and 0.3) by means of broad-band dielectric spectroscopy, differential scanning calorimetry and SQUID magnetometry. We did not confirm the observations of Kumar et al (2009 J. Phys.: Condens. Matter 21 382204), who reported on reversible suppression of ferroelectric polarization in polycrystalline PFW(x)-PZT(1 - x) thin films for magnetic fields above 0.5 T. We did not observe any change of ferroelectric polarization with external magnetic fields up to 3.2 T. Pirc et al (2009 Phys. Rev. B 79 214114) developed a theory explaining the reported large magnetoelectric effect in PFW(x)-PZT(1 - x), taking into account relaxor magnetic and relaxor ferroelectric properties of the system. Our data revealed classical ferroelectric properties below 525 K and 485 K in samples with x = 0.2 and 0.3, respectively. Moreover, paramagnetic behavior was observed down to 4.5 K instead of previously reported relaxor magnetic behavior. It seems that the reported switching-off of ferroelectric polarization in PFW(x)-PZT(1 - x) thin films is not an intrinsic property, but probably an effect of electrodes, interlayers, grain boundaries or second phases presented in polycrystalline thin films.

Soft and central mode behaviour in PbMg(1/3)Nb(2/3)O(3) relaxor ferroelectric.

The relaxor ferroelectric PbMg(1/3)Nb(2/3)O(3) (PMN) is investigated by means of dielectric and Fourier transform far infrared transmission spectroscopy in the frequency range from 10 kHz to 15 THz at temperatures between 20 and 900 K using mostly thin films on infrared transparent sapphire substrates. While the thin film relaxors display reduced dielectric permittivity at low frequencies, their high frequency lattice response is shown to be the same as for single-crystal/ceramic specimens. In contrast to the results of inelastic neutron scattering, the optic soft mode is found to be underdamped at all temperatures. On heating, the TO1 soft phonon follows the Cochran law with an extrapolated critical temperature of 670 K near to the Burns temperature. Above 450 K the soft mode frequency levels off near 50 cm(-1) and above the Burns temperature it slightly hardens. Central-mode-type dispersion assigned to the dynamics of polar nanoclusters appears below the Burns temperature at frequencies near to but below the soft mode and slows down and broadens dramatically on cooling, finally, below the freezing temperature of 200 K, giving rise to frequency independent losses from the microwave range down. A new explanation of the phonon 'waterfall' effect in inelastic neutron scattering spectra is proposed.

Shortening the second phase duration of biphasic shocks: effects of class III antiarrhythmic drugs on defibrillation efficacy in humans.

INTRODUCTION: The specific waveform providing optimal defibrillation threshold (DFT) is unknown. We compared the defibrillation efficacy of biphasic pulses with second phases (P2) of 2 and 5 msec in a randomized prospective clinical study. METHODS AND RESULTS: Intraoperative DFTs of 62 patients (age 54 +/- 13 years; ejection fraction 43% +/- 17%; amiodarone 47%, d,l-sotalol 13%) were determined in random order using a binary search protocol. Anodal shocks of 60% tilt first phases (P1) and P2 of 2 msec/5 msec were delivered from two 100-microF capacitors between the right ventricular electrode and the test housing of a Phylax 06/XM device. Mean DFT was significantly lower using the shorter P2 (9.5 +/- 4.5 J vs 11.3 +/- 5.2 J; P < 0.0001). According to subgroup analysis, the effect of changing P2 duration was only influenced by antiarrhythmic treatment. DFT decreased markedly using the shorter P2 in patients treated with amiodarone (10.7 +/- 4.9 J vs 13.4 +/- 5.6 J; P < 0.00001) or d,l-sotalol (6.1 +/- 3.3 J vs 9.1 +/- 4.6 J; P < 0.05). The difference in patients not treated with Class III drugs was found to be insignificant. Chronic amiodarone treatment increased DFT only when the longer P2 was used. CONCLUSION: Biphasic shocks with shorter P2 should be used in patients undergoing Class III antiarrhythmic treatment.

The influence of short-term treatment with simvastatin on the inflammatory profile of patients with hypercholesterolaemia.

BACKGROUND: Treatment with 3-hydroxy-3-methylglutaryl coenzyme A (HMG CoA) reductase inhibitors can reduce cardiovascular mortality of patients with atherosclerosis. This effect is probably due not only to a decrease in concentration of cholesterol, but also to non-lipid-involving mechanisms elicited by the action of statin drugs. OBJECTIVE: To investigate the influence of short-term therapy with simvastatin on markers of inflammation and oxidation processes in patients with hypercholesterolaemia. DESIGN: We administered 20mg simvastatin daily for 12 weeks to 19 patients with hypercholesterolaemia (250-400 mg/dl). Peripheral blood samples for evaluation of plasma concentrations of thiobarbituric acid reactive substances (malonaldehyde), stable metabolites of nitric oxide (NOx) and interleukin 6 (11-6) were taken before and after the therapy. RESULTS: Plasma levels of malonaldehyde decreased significantly (from 4.533+/-0.428 versus 3.690+/-0.310 micromol/l, P = 0.04) during the study period. Similarly, there was a significant decrease in the plasma concentrations of NOx (from 33.477+/-4.352 micromol/l versus 25.919+/-2.561 micromol/l, P = 0.02). There were significant positive correlations between concentrations of total cholesterol and NOx in plasma (r = 0.4397, P = 0.008) and of low-density lipoprotein and NOx (r = 0.3987, P = 0.02). The plasma level of interleukin 6 remained unchanged by the intervention (1.837+/-0.200 versus 1.820+/-0.169 pg/ml, P = 0.54). CONCLUSIONS: Short-term therapy with simvastatin decreases the plasma concentrations of markers of peroxidation of lipids and of stable metabolites of nitric oxide in hypercholesterolaemic patients, but leaves levels of interleukin 6 unaffected.

[Outstanding contribution of prof. Henryk M. Wisniewski (1931-1999) to the world neuropathology in 20th century]. / Wklad profesora dr. hab. Henryka M. Wisniewskiego (1931-1999) do swiatowej neurologii XX wieku.

Born in Poland in 1931, Henryk Miroslaw Wisniewski, obtained MD at the Medical School in Gdansk (1955), where he continued his neuropathological research awarded with Ph. D. in 1960. During 1961-1962 a worked as a Visiting Scientist at NIH (Institute of Neurology and Communicative Diseases and Stroke). In Medical School in Warsaw he was promoted to Docent degree (an associate professor). In 1966 he emigrated with his family to New York, where he was a Research Associate and Professor at Albert Einstein College of Medicine (1966-1975) Subsequently he became a Director of the State Institute for Basic Research in Developmental Disabilities Staten Island. In New York he remained till his early death at the age of 68. Prof. Wisniewski advanced pathological research concerning the development of dementia, including Alzheimer disease. His investigations proved that presentile dementia (Alzheimer disease) is almost identical with senile dementia. That is why he is called the pioneer of modern Alzheimers research. The comments about his scientific contribution were generously published in scientific journals and daily press. The New York Times cited Dr Mony de Leon Prof. of Psychiatry statement reflecting so well Prof. Wisniewski's achievements "He taught us what the lesions for Alzheimers looked like, what they were made of and how they worked".

The terminal portion of the T wave: a new electrocardiographic marker of risk of ventricular arrhythmias.

Experimental studies have shown that transmural dispersion of repolarization (DoR), defined as the difference in action potential duration between mid-myocardial M-cells, epicardial, and endocardial cells is reflected in the duration of the terminal portion of the T wave (TpTe) on the surface ECG. Since DoR is an important factor associated with the propensity for reentrant arrhythmias, this study examined if TpTe may serve as a marker of risk of ventricular arrhythmias. Data from 18 patients with coronary artery disease and inducible sustained ventricular tachycardia (VT group) were compared with those of 16 survivors of myocardial infarction without inducible VT (control group). TpTe was automatically measured in each beat of 24-hour ECG recordings, and programmed ventricular stimulation was performed in the antiarrhythmic drug-free state. TpTe was expressed as the absolute interval in milliseconds, and relative to the duration of QTe (TpTe/QTe x 100%). TpTe duration was 74 +/- 14 ms in the VT group versus 63 +/- 16 ms in the control group (P < 0.004). The TpTe interval expressed as a percent of the QT interval was 21 +/- 4% in the VT group versus 17 +/- 3% in the control group (P = 0.02). In patients with coronary artery disease. TpTe was longer in patients with, versus without, inducible VT. The results of this study support the hypothesis that TpTe reflects transmural dispersion of repolarization.

Implantation and follow-up of ICD leads implanted in the right ventricular outflow tract.

Unipolar ICD electrodes are routinely implanted at the right ventricular apex (RVA). However, inappropriate pacing/sensing parameters and/or high DFT may limit the appropriateness of the lead's implantation at the RVA. This study examined the effects on DFT of ICD leads implanted in the RVOT, attached to the high interventricular septum as an alternate location. DFT, defibrillation impedance, and sensing and pacing characteristics were measured at the time of implantation in 28 consecutive patients. Group A consisted of 12 patients in whom the ICD implantation criteria in the RVA were not satisfied, and whose lead was placed in the RVOT. Group B consisted of 16 patients with ICD electrodes implanted at the RVA. Mean DFT in group A was 11 +/- 4 J (4.5-20 J) versus 12 +/- 6 J (4-20 J) in the group B (P = 0.58). Defibrillation impedance was 81 +/- 9 omega (69-92 omega) in group A versus 77 +/- 15 omega) (46-93 omega) in group B (P = 0.43). R wave amplitude, slew rate, pacing threshold, and pacing impedance were comparable in both groups. In the perioperative period, the electrode needed to be repositioned in two patients from group A. There was no further dislodgment of RVOT defibrillation leads or other lead related complications during a follow-up of 23 +/- 9 months. The placement of ICD leads in the RVOT is an alternative to the RVA position. However, active-fixation ICD leads should be considered to limit the risk of electrode dislodgment.

Fibrinolytic therapy and n-acetylocysteine in the treatment of patients with acute myocardial infarction: its influence on authentic plasma hydroperoxide levels and polymorphonuclear neutrophil oxygen metabolism.

Recently it has been demonstrated that the administration of n-acetylocysteine (NAC), in combination with streptokinase, significantly diminished oxidative stress in patients with myocardial infarction. The aim of our study was to assess the influence of NAC treatment, as adjunct therapy in an evolving myocardial infarction, on the polymorphonuclear count, superoxide anion and hydrogen peroxide levels and nitric oxide production by PMNs and authentic plasma hydroperoxide (ROOH). Treatment of patients with NAC in addition to reperfusion therapy was accompanied by a significant decrease in the number of circulating polymorphonuclear neutrophils. However, the oxygen metabolism of PMNs was not affected by NAC administration. The concentration of authentic plasma hydroperoxide was significantly reduced by the administration of NAC which suggests diminished oxidative stress during acute myocardial infarction.

Electrical atrial remodeling assessed by monophasic action potential and atrial refractoriness in patients with structural heart disease.

UNLABELLED: The present study was performed to assess the effect of induced atrial fibrillation (AF) on atrial monophasic action potentials (MAPs) and atrial refractory period (ERP) in patients with structural heart disease. An electrode MAP catheter was placed in the right atrium to continuously measure atrial potential duration (APD90) in 13 patients (coronary artery disease, 10 patients; dilated cardiomyopathy, 2 patients; hypertrophic cardiomyopathy, 1 patient) without spontaneous AF episodes. AF was induced by rapid atrial stimulation (300-1500/min). If sinus rhythm returned within 10 minutes, AF was reinduced. The atrial ERP was measured during atrial pacing at a basic cycle length of 550 ms before AF induction and after its conversion. RESULTS: The mean atrial ERP and the atrial APD90 before AF was 242 +/- 34 ms and 256 +/- 23 ms, respectively. ERP and APD90 shortening was observed after 3 minutes of AF. After 11 +/- 0.5 min (10 min 20 s-13 min 10 s) of AF, ERP and APD90 reached their minimal values of 72% +/- 13% and 71% +/- 10% of baseline, respectively. ERP and APD90 returned to their initial values within 10 minutes after conversion of AF. A tendency toward longer duration of consecutive AF episodes and facilitation of their induction was observed. CONCLUSION: The present study confirms that short episodes of AF modify the electrophysiological properties of the atria in humans. In patients with structural heart disease, induced atrial fibrillation shortens the atrial ERP as well as the atrial APD90. The changes were reversible within 10 minutes after arrhythmia termination.

[Andrew Victor Schally: neuroendocrinologist of Polish origin]. / Andrew Victor Schally--zasluzony neuroendokrynolog Polskiego pochodzenia.

American scientist of Polish origin, won the Nobel Prize in the field of physiology and medicine. In this way he became one of three Polish Nobel Prize winners in the scientific field (among M. Sklodowska-Curie and Tadeusz Reichstein). On the 20th anniversary of this historic moment I describe his life, scientific activity and achievements.

[Henryk Jordan (1842-1907)--a dedicated Krakow physician, health promotor and welfare worker]. / Henryk Jordan (1842-1907)--zasluzony krakowski lekarz, promotor zdrowia i spolecznik.

The article presents Dr Jordan's life and professional career. His pioneering has been realized not only in Poland but in other European countries as well.

New insight into repolarization abnormalities in patients with congenital long QT syndrome: the increased transmural dispersion of repolarization.

There is evidence from experimental studies that the time interval from the peak to the end of T-wave reflects the transmural dispersion in repolarization (electrical gradient) between myocardial "layers" (epicardial, M-cells, endocardial). Since Congenital Long QT Syndrome (LQTS) is considered to be classical disease or repolarisation abnormalities, we performed the present study to assess the transmural dispersion of repolarization in LQTS patients. The study group consisted of 17 patients: 7 LQTS pts and 10 pts from the control group. In each patient the 24-hour ECG recording was performed on magnetic tape. The interval from the peak to the end of the T-wave (TpTo) was automatically measured by Holter system during every hour as a measure of transmural dispersion of repolarisation. Thereafter the mean TpTo from 24-hours was calculated. In addition the spatial QT dispersion was measured from 12 lead ECG and 3 channel Holter tape as a difference between the shortest and the longest QT interval between leads. The values were compared between groups using the Anova test. TpTo was 79.6 +/- 9.6 ms (72-92 ms) in LQTS group and 62.4 +/- 7.5 ms (51-70) in the control group (p < 0.001). In LQTS group TpTo was significantly longer at night hours 72.5 +/- 2 when compared to day hours 87.4 +/- 8 (p < 0.01). The spatial QT dispersion was significantly higher in LQTS patients when compared to control, both in 12-lead standard and Holter ECG. Congenital long QT syndrome is associated with increase in both transmural and spatial dispersion of repolarization. The extent of prolongation of the terminal portion of QT in patients with congenital long QT syndrome is greater at night sleep hours compared to daily activity.

[The application of lead in pharmacotherapy in time past and today]. / Wykorzystanie olowiu w farmakoterapii dawniej i dzis.

The review of literature shows that lead and its compounds accompany man from the beginning of mankind to present days. In the evolution of the therapeutic use of lead we can discern the periods of a fascination for its compounds, e.g. the antique, especially in Rome, and the galenic period up to the XVIII century. The development of chemistry, toxicology and pharmacology at the breach of XVIII and XIX century led to a limitation of lead use in the therapy. It must be emphasized that it never came to a resignation. It remains still an element of the traditional pharmacotherapy in many cultures, e.g. of Hindus, Westafricans and Mexicans.