ライフサイエンスコーパス: acoustic pressure

1 e area, potentially the entire brain, at low acoustic pressure.

2 tion and are directly related to the applied acoustic pressure.

3 finity microbubble concentrations at various acoustic pressures.

4 diameter of 4.3 um) using ultrasound pulses (acoustic pressure 0.034 MPa, center frequency 1.24 MHz a

5 Two different acoustic pressures, 0.25 and 0.83 MPa, were simulated fo

6 ls did extravasate when using the two higher acoustic pressures, 0.53 and 0.71 MPa, immediately after

7 duced by gas vesicles as they collapse under acoustic pressure above a threshold defined by the ARG.

8 rs include the number of active bubbles, the acoustic pressure acting on each bubble and the bubble s

9 duced without evident tissue damage, and the acoustic pressure amplitude where the probability for BB

10 on of acoustic pulse position, duration, and acoustic pressure amplitude.

11 ting superior cavitation properties at lower acoustic pressure amplitudes.

12 for transmitting vibrations originating from acoustic pressure and active outer hair cell force to th

13 Additionally, excessive acoustic pressure and high temperature from HIFU generat

14 g how the organ of Corti vibrates because of acoustic pressure and outer hair cell force is critical

15 which was directly explained by the applied acoustic pressure and the brain functional connectivity

16 Higher acoustic pressures and longer cycles resulted in more di

17 e in the observed effects on cells, and that acoustic pressure appears to be concurrent with, but not

18 =0.05) than that of free microbubbles at all acoustic pressures applied.

19 Keeping the acoustic pressure at levels where no such sign of microb

20 hich is associated with temperature rise and acoustic pressure; (b) simulation of stochasticity of SU

21 of small (<1nm) molecules has been shown at acoustic pressures below 1MPa both in vitro and in vivo,

22 ransgenic and non-transgenic mice at similar acoustic pressures but exhibited different leakage kinet

23 Increasing the acoustic pressure can extend the use of rapid short-puls

24 mall" MBs with a moderate level (0.6 MPa) of acoustic pressure can further enhance these effects.

25 positive acoustic contrast, at a node in the acoustic pressure distribution while aligning the negati

26 ional degrees of freedom for emulating spin, acoustic pressure field is scalar in nature, and it requ

27 uss how both time-averaged and instantaneous acoustic pressure fields can affect the integrity of sur

28 yrene microbead as a function of the applied acoustic pressure for a better understanding of the rela

29 Our results show that acoustic pressures had the strongest effect on cavitatio

30 zoelectric effect in the solid substrate and acoustic pressure in the fluid, was developed to provide

31 ables continuous monitoring of intracochlear acoustic pressure locally, which could improve cochlear

32 The external stimulation is acoustic pressures mediated by the scala fluids, whereas

33 and bioluminescence imaging to optimize the acoustic pressure, microbubble concentration, treatment

34 from clouds of cavitating bubbles at higher acoustic pressures (multi-bubble sonoluminescence) is do

35 ates within a narrow therapeutic window, the acoustic pressure needs to be adjusted to factor in a hi

36 ic radiation force and are pushed toward the acoustic pressure node.

37 rapid short-pulses are versatile and, at an acoustic pressure of 0.35 MPa, can deliver therapeutics

38 asured TMC to be 0.106+/-0.032mum (n=70) for acoustic pressure of 1.5MPa (duration 13.3mus), and incr

39 nd increased to 0.171+/-0.030mum (n=125) for acoustic pressure of 1.7MPa and to 0.182+/-0.052mum (n=1

40 However, the ability to fully control the acoustic pressure profile over its propagation path has

41 entrations) and ultrasound properties (e.g., acoustic pressure, pulse duration).

42 etration depth of nanocarriers using various acoustic pressures, ranging between 1.7 and 6.9MPa.

43 lications, in particular with respect to the acoustic pressures required for activation, thereby mini

44 distinguished from each other based on their acoustic pressure-response profiles, enabling 'two-tone'

45 The acoustic pressure threshold needed for PFH-NDs vaporizat

46 se observations, our group characterized the acoustic pressure transients generated by nsEP and deter

47 own spectroscopy event can be recorded as an acoustic pressure wave to obtain information related to

48 Acoustic pressure waves can impose radiation force on a

49 Intravascular lithotripsy (IVL) delivers acoustic pressure waves to modify calcium, enhancing ves

50 phy (MSOT) uses pulsed laser light to induce acoustic pressure waves, enabling the visualization of e

51 stic transducer (PIAT) designed to sense the acoustic pressure while fully implanted inside a living

52 intravenously injected microbubbles at a low acoustic pressure without inducing BBB opening.