Abstract:Ultrasound is used extensively in medical imaging and therapy, non‐destructive testing, flow sensing, underwater range assessment, and acoustic microscopy. To ensure the accuracy of these techniques, detailed knowledge of the acoustic pressure field produced by the ultrasonic transducer is required. This paper proposes a functional polymer membrane loaded with ultrasound‐activated luminescent microparticles. The semitransparent membrane makes use of the luminescent properties of BaSi2O2N2:Eu2+ to convert ultra… Show more
“…[ 2 ] Correlations between the level of applied stress and the intensity of luminescence enable a variety of applications, [ 3 , 4 ] for example, in stress sensors, crack detectors, or smart displays. [ 5 , 6 , 7 , 8 , 9 , 10 ] ML induced by ultrasonic excitation (USML) was evaluated for the ability to visualize ultrasonic power distribution, [ 11 , 12 ] but also for security and anticounterfeiting purposes, [ 13 ] or as a photon source in photocatalysis, [ 14 ] photobioreactors, [ 15 ] and optogenetics. [ 16 ] In comparison to conventional ML excited by static or tactile forces, USML offers a remote trigger for luminescent light emission; however, it is currently much less exploited.…”
Ultrasound‐induced mechanoluminescence (USML) of Erbium‐doped CaZnOS is reported. Using the fluorescence intensity ratio of the
2
H
11/2
,
4
S
3/2
→
4
I
15/2
transitions of Er
3+
allows for simultaneous temperature mapping at an absolute sensitivity of 0.003 K
−1
in the physiological regime. The combination of USML, local heating, and remote read‐out enables a feedback and response loop for highly controlled stimulation. It is found that ML is a result of direct energy transfer from the host material to Er
3+
, giving room for adapted spectral characteristics through bandgap modulation. ML saturation at high acoustic power enables independent control of local light emission and ultrasonic heating. Such USML materials may have profound implications for optogenetics, photodynamic therapy and other areas requiring local illumination, heating, and thermometry simultaneously.
“…[ 2 ] Correlations between the level of applied stress and the intensity of luminescence enable a variety of applications, [ 3 , 4 ] for example, in stress sensors, crack detectors, or smart displays. [ 5 , 6 , 7 , 8 , 9 , 10 ] ML induced by ultrasonic excitation (USML) was evaluated for the ability to visualize ultrasonic power distribution, [ 11 , 12 ] but also for security and anticounterfeiting purposes, [ 13 ] or as a photon source in photocatalysis, [ 14 ] photobioreactors, [ 15 ] and optogenetics. [ 16 ] In comparison to conventional ML excited by static or tactile forces, USML offers a remote trigger for luminescent light emission; however, it is currently much less exploited.…”
Ultrasound‐induced mechanoluminescence (USML) of Erbium‐doped CaZnOS is reported. Using the fluorescence intensity ratio of the
2
H
11/2
,
4
S
3/2
→
4
I
15/2
transitions of Er
3+
allows for simultaneous temperature mapping at an absolute sensitivity of 0.003 K
−1
in the physiological regime. The combination of USML, local heating, and remote read‐out enables a feedback and response loop for highly controlled stimulation. It is found that ML is a result of direct energy transfer from the host material to Er
3+
, giving room for adapted spectral characteristics through bandgap modulation. ML saturation at high acoustic power enables independent control of local light emission and ultrasonic heating. Such USML materials may have profound implications for optogenetics, photodynamic therapy and other areas requiring local illumination, heating, and thermometry simultaneously.
“…US heating activates the release of pPL trap states, leading to TSL emission. [22] Cyclic US stimulation data are presented in Figure 4 for rapid cycling (Figure 4e) and slow cycling (Figure 4f ). In both cases, cycles are sufficiently short to avoid any saturation effects: the temperature increase generated on the GCC by each cycle is on the order of 3 K (in comparison to about 30 K in the quasistatic experiments reported in Figure 3).…”
Section: Resultsmentioning
confidence: 99%
“…[18][19][20][21] Polymer membranes with embedded USL particles were used for fast visualization of the cross-section of ultrasound pressure fields with a spatial resolution below 200 μm for acoustic pressures in the range of 150-4,500 kPa, and frequencies of 1-25 MHz. [22] Such applications could notably benefit from the enhanced mechanical stiffness, thermal stability, and spatial homogeneity offered by fully inorganic ceramics and ceramic composites.…”
“…Quite often the persistent luminescence and thermoluminescence of these materials can be adequately modeled using a set of discrete trap depths obeying first-order kinetics. [159][160][161] Additionally there is also a lack of physical grounds behind the use of higher-order kinetics to fit TL glow curves that result from an underlying trap distribution and hence this should be avoided. [162,163] Multiple measurement and analysis protocols have been developed over the years to extract trap depths and frequency factors of the corresponding traps in the material.…”
Section: Thermoluminescencementioning
confidence: 99%
“…One notable example is the recent discovery that the light emitted by a persistent phosphor under exposure to an ultrasound beam is in fact not due to mechanical stimulation as was first conjectured, [237] but is essentially due to local ultrasonic heating and is hence a special form of thermoluminescence. [160,161]…”
Glow-in-the-dark materials have been around for a long time. While formerly materials had to be mixed with radioactive elements to achieve a sufficiently long and bright afterglow, these have now been replaced by much safer alternatives. Notably strontium aluminate, SrAl 2 O 4 , doped with europium and dysprosium, has been discovered over two decades ago and since then the phosphor has transcended its popular use in watch dials, safety signage, or toys with more niche applications such as stress sensing, photocatalysis, medical imaging, or flicker-free light-emitting diodes. A lot of research efforts are focused on further improving the storage capacity of SrAl 2 O 4 :Eu 2+ ,Dy 3+ , including in nanosized particles, and on finding the underlying physical mechanism to fully explain the afterglow in this material and related compounds. Here an overview of the most important results from the research on SrAl 2 O 4 :Eu 2+ ,Dy 3+ is presented and different models and the underlying physics are discussed to explain the trapping mechanism at play in these materials.
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