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Pulse Rate

Pulse Rate is the measurement of the number of times the heart beats per unit of time, typically expressed as beats per minute (bpm).
This vital sign provides valuable insights into the cardiovascular health and overall physiological state of an individual.
Factors such as age, physical activity, emotions, and certain medical conditions can influence pulse rate.
Accurately measuring and monitoring pulse rate is crucial for healthcare professionals when assessing a patient's condition, detecting abnormalities, and guiding appropriate medical interventions.
The PubCompare.ai platform can optimize pulse rate research by helping researchers locate the best protocols from literature, preprints, and patents, while using advanced comparisons to enhance reproducibility and accuarcy.
Leveraging artificial intelligence, PubCompare.ai takes the guesswork out of your research and ensures you find the most reliable and effective protocols for your pulse rate studies.

Most cited protocols related to «Pulse Rate»

1
Photoelectron Momentum Distribution of Neon Dimer
Starting from a 2p atomic orbital aligned along the molecular axis, we solve the three-dimensional TDSE in single-active-electron approximation with the split-operator method on a Cartesian grid with 512 points in each dimension, a grid spacing of 0.25 a.u. and a time step of 0.02 a.u. While propagating up to a final time T = 1500 a.u., outgoing parts of the wave function are projected onto Volkov states44 (link). The potential for a single neon atom is chosen as in ref. 45 (link) but with the singularity removed using a pseudopotential46 (link) for angular momentum l = 1. The clockwise circularly polarized pulse has a 12-cycle sin2 envelope and a peak field strength of 0.096 a.u. To obtain the momentum distribution for the dimer we multiply two copies of the atomic distribution by e±ik·R/2, respectively (|R|/2 = 2.93 a.u.) and then add them coherently with an additional factor of ± 1 depending on the type of interference, gerade, or ungerade. To account for different possible orientations of the dimer with respect to the polarization plane, we vary the angle between them in 8 steps to cover a range from 0 to 45°, project the molecular photoelectron momentum distribution (PMD) onto the polarization plane and add these projections together with their geometrical weights. The PMDs are then averaged over the ATI peaks to obtain the final distributions shown in Fig. 2.
Kunitski M., Eicke N., Huber P., Köhler J., Zeller S., Voigtsberger J., Schlott N., Henrichs K., Sann H., Trinter F., Schmidt L.P., Kalinin A., Schöffler M.S., Jahnke T., Lein M, & Dörner R. (2019). Double-slit photoelectron interference in strong-field ionization of the neon dimer. Nature Communications, 10, 1.
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Publication 2019
Electrons Epistropheus Mental Orientation Neon Persistent Mullerian duct syndrome Pulse Rate
2
Calculating Relative Efficiency in CASL
All image data were saved as raw echo intensities and reconstructed offline with custom software. Partial Fourier raw data was acquired at lines –m ≤ u ≤ N/2 (m = 6, N= 64). The low frequency phase map of each coil was estimated from the Fourier transformation of the image generated by Hanning filtering the center portion of the raw data at lines –m ≤ u ≤ m. The final image was combined from each coil image, weighted by the conjugate of the corresponding low resolution phase map. A Region of interest (ROI) for each subject was defined to contain the entire brain.
For the first study, the relative combined inversion efficiency was defined as the ratio of the PCASL average difference signal when control and label are set below the brain to the average CASL difference signal after compensating for the duty cycle difference (dividing the CASL difference signal by dcycle). dcycle is the duty cycle of continuous ASL, which is 53.33% in our study. Previous simulations of adiabatic fast passage demonstrate that the labeling efficiency may not have a linear relationship with the RF duty cycle in the pulsed-form CASL(32 (link)). Simulation was performed to calculate the mean labeling efficiency for the laminar flow across the different time when spin passes through the labeling plane. The simulation result shows that the relative efficiency is within 2% difference with the RF duty cycle. This linearity between the RF duty cycle and labeling efficiency is likely valid because of the long pulse period (375 ms) used in the CASL sequence. This improvement with longer labeling blocks (A pulse period of 100 ms was better approximated by a linear relationship than a pulse period of 20 ms) was suggested in previously reported simulations (32 (link)). The relative efficiency loss of the control pulse was defined as the ratio of the PCASL average difference signal when the control is set below the brain compared with above the brain to the average CASL difference signal after compensating for the duty cycle difference. Because of the very low SNR in the average difference signal between controls in PCASL, we used the low-resolution phase map from the average difference signal between control and label when applied below the brain to phase correct the images from each coil. The relative systematic error between control and label pulses was defined as the ratio of the average PCASL difference signal between control and label when applied above the brain to the average CASL difference signal after compensating for the duty cycle difference. The relative efficiency of labeling pulse was defined as the ratio of the PCASL average difference signal when the label is set below the brain compared with above the brain to the average CASL difference signal after compensating for the duty cycle difference. We used low-resolution phase maps to correct the phase of the image from each coil as in the relative efficiency calculation of control pulse.
For the second study the relative combined efficiency described for the first study was employed. For the third study, frequency-dependent off-resonance saturation effects were analyzed by averaging the difference images (between the control and label images) across the phase direction.
Dai W., Garcia D., de Bazelaire C, & Alsop D.C. (2008). Continuous Flow Driven Inversion for Arterial Spin Labeling Using Pulsed Radiofrequency and Gradient Fields. Magnetic resonance in medicine : official journal of the Society of Magnetic Resonance in Medicine / Society of Magnetic Resonance in Medicine, 60(6), 1488-1497.
Publication 2008
Brain ECHO protocol Inversion, Chromosome Microtubule-Associated Proteins Pulse Rate Pulses Spin Labels Vibration
3
GABA-Edited MRS in Healthy Adults
To demonstrate the utility of the Gannet software, GABA-edited spectra were acquired in 10 healthy adult volunteers, who provided written informed consent with the approval of the Cardiff University School of Psychology ethics board. In each subject, spectra (repeated four times) were acquired for each of three brain regions: occipital (OCC; including primary visual cortex); sensorimotor (SM; including primary somatosensory and motor cortex); and dorsolateral prefrontal (DLPF), as shown in Figure 3. Experimental parameters were relatively standard for the field (2 (link)), including: GE Signa HDx 3 Tesla (T) scanner using an eight-channel phased-array head coil for receive; repetition time (TR) 1.8 s; echo time (TE) 68 ms; 332 transients of 4k datapoints sampled at 5 kHz; 16 ms Gaussian editing pulse with 95 Hz bandwidth applied at 1.9 ppm in ON scans and 7.46 ppm in OFF scans in an interleaved manner; voxel size 3 × 3 × 3 cm3; acquisition time 10 min. Data were acquired on a GE Signa HDx 3T scanner; a two-step phase cycle, which was time averaged on the scanner so that each FID in the exported data represented two TRs or a period of 3.6 s. OFF/ON interleaving of editing was performed outside the phase cycle loop, so that lines of the exported data were alternately OFF, ON, etc. The unsuppressed water signals from the same volumes were also acquired for quantification.
As mentioned above these GABA+-edited data contain substantial contributions from macromolecular contaminants, which can be removed by a symmetrical editing scheme (22 (link),23 (link)). To demonstrate the ability of Gannet to model MM-suppressed GABA spectra, data were acquired at a TE of 80 ms (22 (link)) in a single healthy subject with 20 ms editing pulses at 1.9 ppm (ON scans) and 1.5 ppm (OFF scans). Other experimental parameters include: TR 2 s; 2k datapoints sampled at 2 kHz; 3 × 3 × 3 cm3 voxel in a primary sensorimotor region (4 (link)).
Edden R.A., Puts N.A., Harris A.D., Barker P.B, & Evans C.J. (2013). Gannet: A Batch-Processing Tool for the Quantitative Analysis of Gamma-Aminobutyric Acid–Edited MR Spectroscopy Spectra. Journal of magnetic resonance imaging : JMRI, 40(6), 1445-1452.
Publication 2013
Adult Brain ECHO protocol gamma Aminobutyric Acid Head Healthy Volunteers Motor Cortex Pulse Rate Pulses Radionuclide Imaging Striate Cortex Transients
4
CEST Imaging of Glycogen Phantom and Calf Muscle
All images were acquired using a whole-body Philips 3T Achieva scanner (Philips Medical System, Best, The Netherlands) equipped with 80 mT/m gradients. RF was transmitted using the body coil and SENSE reception (31 (link)) was employed. A series of consecutive direct saturation and CEST scans were performed using the 8-element knee coil for both the glycogen phantom and in vivo human calf muscle. To minimize leg motion, foam padding was placed between the subject’s lower leg and the knee coil. In all cases, second order shims over the entire muscle on the imaging slice were optimized to minimize B0 field inhomogeneity. Notice that the width of Z-spectra depends on T2 and that the WASSR procedure provides an absolute field frequency map so that there is no need for higher order shimming for the CEST acquisition. Clinical imagers generally employ a prescan to center the bulk water signal of the object/subject, optimize the flip angle and shim the field. Note that no such “prescan” should be made between direct saturation and CEST scans to maintain the same field reference conditions. For both scans, saturation was accomplished using a rectangular RF pulse before the turbo spin echo (TSE) image acquisition, as previously described by Jones et al. (21 (link)).
The power level needed for each saturation experiment depended on the load and was optimized by measuring sets of Z-spectra under these different conditions. For WASSR, the power and pulse lengths were chosen as small as possible to have sufficient direct saturation, while minimizing any MT effects. For CEST, the maximum pulse length allowed for the body coil within the protected clinical software (500 ms) was used and the power was optimized for maximum effect at the phantom and muscle loads. WASSR was obtained at higher frequency resolution than CEST, but over a smaller frequency range as only the direct saturation region needs to be covered. The WASSR range was chosen sufficiently large to validate the simulated results, consequently leading to a larger number of frequencies needed in vivo than for the phantom.
Single-slice glycogen phantom imaging was performed using SENSE factor = 2, TSE factor [number of refocusing pulses] = 34 (two-shots TSE), TR = 3000 ms, TE = 11 ms, matrix = 128 × 122, FOV = 100 × 100 mm2, slice thickness = 5 mm, NSA = 1. Imaging parameters for human calf muscle experiments were identical to those in phantom experiments except for the following: FOV = 160 × 160 mm2. The saturation spectral parameters for WASSR and CEST are indicated in Table 1.
Kim M., Gillen J., Landman B.A., Zhou J, & van Zijl P.C. (2009). WAter Saturation Shift Referencing (WASSR) for chemical exchange saturation transfer experiments. Magnetic resonance in medicine : official journal of the Society of Magnetic Resonance in Medicine / Society of Magnetic Resonance in Medicine, 61(6), 1441-1450.
Publication 2009
Dietary Fiber ECHO protocol Glycogen Homo sapiens Human Body Knee Joint Leg Muscle Tissue Pulse Rate Pulses Radionuclide Imaging SHIMS
5
Comprehensive Neuronal Tracing and Characterization
For in situ hybridization analysis, cryostat sections were hybridized using digoxigenin-labeled probes [45 (link)] directed against mouse TrkA or TrkB, or rat TrkC (gift from L. F. Parada). Antibodies used in this study were as follows: rabbit anti-Er81 [14 (link)], rabbit anti-Pea3 [14 (link)], rabbit anti-PV [14 (link)], rabbit anti-eGFP (Molecular Probes, Eugene, Oregon, United States), rabbit anti-Calbindin, rabbit anti-Calretinin (Swant, Bellinzona, Switzerland), rabbit anti-CGRP (Chemicon, Temecula, California, United States), rabbit anti-vGlut1 (Synaptic Systems, Goettingen, Germany), rabbit anti-Brn3a (gift from E. Turner), rabbit anti-TrkA and -p75 (gift from L. F. Reichardt), rabbit anti-Runx3 (Kramer and Arber, unpublished reagent), rabbit anti-Rhodamine (Molecular Probes), mouse anti-neurofilament (American Type Culture Collection, Manassas, Virginia, United States), sheep anti-eGFP (Biogenesis, Poole, United Kingdom), goat anti-LacZ [14 (link)], goat anti-TrkC (gift from L. F. Reichardt), and guinea pig anti-Isl1 [14 (link)]. Terminal deoxynucleotidyl transferase-mediated biotinylated UTP nick end labeling (TUNEL) to detect apoptotic cells in E13.5 DRG on cryostat sections was performed as described by the manufacturer (Roche, Basel, Switzerland). Quantitative analysis of TUNEL+ DRG cells was performed essentially as described [27 (link)]. BrdU pulse-chase experiments and LacZ wholemount stainings were performed as previously described [46 (link)]. For anterograde tracing experiments to visualize projections of sensory neurons, rhodamine-conjugated dextran (Molecular Probes) was injected into single lumbar (L3) DRG at E13.5 or applied to whole lumbar dorsal roots (L3) at postnatal day (P) 5 using glass capillaries. After injection, animals were incubated for 2–3 h (E13.5) or overnight (P5). Cryostat sections were processed for immunohistochemistry as described [14 (link)] using fluorophore-conjugated secondary antibodies (1:1,000, Molecular Probes). Images were collected on an Olympus (Tokyo, Japan) confocal microscope. Images from in situ hybridization experiments were collected with an RT-SPOT camera (Diagnostic Instruments, Sterling Heights, Michigan, United States), and Corel (Eden Prairie, Minnesota, United States) Photo Paint 10.0 was used for digital processing of images.
Hippenmeyer S., Vrieseling E., Sigrist M., Portmann T., Laengle C., Ladle D.R, & Arber S. (2005). A Developmental Switch in the Response of DRG Neurons to ETS Transcription Factor Signaling. PLoS Biology, 3(5), e159.
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Publication 2005
Anabolism Animals Antibodies Apoptosis Bromodeoxyuridine Calbindins Calretinin Capillaries Cavia Cells Diagnosis Digoxigenin DNA Nucleotidylexotransferase Domestic Sheep Goat Immunohistochemistry In Situ Hybridization In Situ Nick-End Labeling LacZ Genes Lumbar Region Mice, House Microscopy, Confocal Molecular Probes Neurofilaments Neuron, Afferent Pulse Rate Rabbits Rhodamine rhodamine dextran Root, Dorsal Staining transcription factor PEA3 tropomyosin-related kinase-B, human

Most recents protocols related to «Pulse Rate»

1
Indium Oxide Thin Film Deposition by ALD
Not available on PMC !

Example 1

InCl (1 eq.) was added to a Schlenk flask charged with LiCp(CH2)3NMe2 (11 mmol) in Et2O (50 mL). The reaction mixture was stirred overnight at room temperature. After filtration of the reaction mixture, the solvent was evaporated under reduced pressure to obtain a red oil. After distillation a yellow liquid final product was collected (mp˜5° C.). Various measurements were done to the final product. 1H NMR (C6D6, 400 MHz): δ 5.94 (t, 2H, Cp-H), 5.82 (t, 2H, Cp-H), 2.52 (t, 2H, N—CH2—), 2.21 (t, 2H, Cp-CH2—), 2.09 (s, 6H, N(CH3)2, 1.68 (q, 2H, C—CH2—C). Thermogravimetric (TG) measurement was carried out under the following measurement conditions: sample weight: 22.35 mg, atmosphere: N2 at 1 atm, and rate of temperature increase: 10.0° C./min. 97.2% of the compound mass had evaporated up to 250° C. (Residue <2.8%). T (50%)=208° C. Vacuum TG measurement was carried out under delivery conditions, under the following measurement conditions: sample weight: 5.46 mg, atmosphere: N2 at 20 mbar, and rate of temperature increase: 10.0° C./min. TG measurement was carried out under delivery conditions into the reactor (about 20 mbar). 50% of the sample mass is evaporated at 111° C.

Using In(Cp(CH2)3NMe2) synthesized in Example 1 as an indium precursor and H2O and O3 as reaction gases, indium oxide film may be formed on a substrate by ALD method under the following deposition conditions. First step, a cylinder filled with In(Cp(CH2)3NMe2) is heated to 90° C., bubbled with 100 sccm of N2 gas and the In(Cp(CH2)3NMe2) is introduced into a reaction chamber (pulse A). Next step, O3 generated by an ozone generator is supplied with 50 sccm of N2 gas and introduced into the reaction chamber (pulse B). Following each step, a 4 second purge step using 200 sccm of N2 as a purge gas was performed to the reaction chamber. 200 cycles were performed on a Si substrate having a substrate temperature of 150° C. in the reaction chamber at a pressure of about 1 torr. As a result, an indium oxide film will be obtained at approximately 150° C.

Example 2

Same procedure as Example 1 started from Li(CpPiPr2) was performed to synthesize In(CpPiPr2). An orange liquid was obtained. 1H NMR (C6D6, 400 MHz): δ 6.17 (t, 2H, Cp-H), 5.99 (t, 2H, Cp-H), 1.91 (sept, 2H, P—CH—), 1.20-1.00 (m, 12H, C—CH3).

Using In(CpPiPr2) synthesized in Example 2 as the indium precursor and H2O and O3 as the reaction gases, indium oxide film may be formed on a substrate by the ALD method under the following deposition conditions. First step, a cylinder filled with In(CpPiPr2) is heated to 90° C., bubbled with 100 sccm of N2 gas and the In(CpPiPr2) is introduced into a reaction chamber (pulse A). Next step, O3 generated by an ozone generator is supplied with 50 sccm of N2 gas and introduced into the reaction chamber (pulse B). Following each step, a 4 second purge step using 200 sccm of N2 as a purge gas was performed to the reaction chamber. 200 cycles were performed on the Si substrate having a substrate temperature of 150° C. in an ALD chamber at a pressure of about 1 torr. As a result, an indium oxide was obtained at 150° C.

US11859283B2. Heteroalkylcyclopentadienyl indium-containing precursors and processes of using the same for deposition of indium-containing layers (2024-01-02). L'Air Liquide, Société Anonyme pour l'Etude et l'Exploitation des Procédés Georges Claude [FR]. Inventors: Antoine Bruneau [FR], Takashi Ono [JP], Christian Dussarrat [JP].
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Patent 2024
1H NMR Atmosphere Distillation Fever Filtration Indium indium oxide Obstetric Delivery Ozone Pressure Pulse Rate Solvents Vacuum
2
Hafnium Metal Production from Hafnium Chloride
Not available on PMC !

Example 5

113 g of sodium metal was melted and brought to 250° C. in an Inconel reactor vessel. The sodium was then stirred using a Cowles blade mixer rotating at 2000-2500 rpm. Powdered hafnium chloride (from Areva) was pulse-fed over approximately 1 hour into the stirred sodium, until 82 g of hafnium chloride had been added, at which point the reaction was halted. At the end of the reaction, the vortex in the sodium had substantially disappeared and the reactor temperature had increased to 301° C.

Once the reaction was completed, the reactor vessel was sealed, transferred to a furnace, and heated to 825° C. for four hours to reduce the surface area of the hafnium metal produced in the reaction. During this process step, unreacted sodium was removed from the hafnium metal to leave a hafnium-sodium chloride composite.

The hafnium and sodium chloride mixture was then transferred to a vacuum furnace and heated under vacuum to 2300° C., held at that temperature for one hour, and then cooled. This removed the sodium chloride and produced a button of solid hafnium.

The hafnium button was analyzed via glow discharge mass spectrometry (GDMS) and found to have 26 ppm oxygen content, 1690 ppm zirconium, and less than 150 ppm total transition metals. The results demonstrate the production of a low oxygen hafnium metal produced directly from hafnium powder consolidation.

US11858046B2. Methods for producing metal powders (2024-01-02). Nanoscale Powders LLC [US]. Inventors: David Henderson [US], Andrew Matheson [US], Richard Van Lieshout [US], Donald Finnerty [US], John W. Koenitzer [US].
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Patent 2024
ARID1A protein, human Blood Vessel Hafnium hafnium chloride Mass Spectrometry Metals Oxygen Patient Discharge Powder Pulse Rate Sodium Sodium Chloride Transition Elements Vacuum Zirconium
3
Retinal Vein Occlusion Mouse Model
Not available on PMC !

Example 2

In the following experiments, a mouse model of RVO, which induces reproducible retinal edema was used. RVO is the model that was used for testing anti-VEGF therapies for DME. Brown et al., Ophthalmology 117, 1124-1133 el 121 (2010); and Campochiaro et al., Ophthalmology 117, 1102-1112 e1101 (2010). I n this model, Rose Bengal, a photoactivatable dye, is injected into the tail veins of adult C57B16 mice and photoactivated by laser of retinal veins around the optic nerve head. A clot is formed and edema or increased retinal thickness develops rapidly. Inflammation, also seen in diabetes, also develops.

Fluorescein leakage and maximal retinal edema, measured by fluorescein angiography and optical coherence tomography (OCT), respectively, using the Phoenix Micron IV, is observed 24 h after RVO. Retinal edema is maintained over the first 3 days RVO. By day 4 the edema decreases and the retina subsequently thins out. In addition to edema formation there is evidence of cell death in the photoreceptor cell layer by day 2 after RVO.

In this example, mice were anesthetized with intra-peritoneal (IP) injection of ketamine and xylazine. One drop of 0.5% alcaine was added to the eye as topical anesthetic. The retina was imaged with the Phoenix Micron IV to choose veins for laser ablation using the Phoenix Micron IV image guided laser. One to four veins around the optic nerve head were ablated by delivering a laser pulse (power 50 mW, spot size 50 μm, duration 3 seconds) to each vein.

US11857609B2. Ocular delivery of cell permeant therapeutics for the treatment of retinal edema (2024-01-02). THE TRUSTEES OF COLUMBIA UNIVERSITY IN THE CITY OF NEW YORK [US]. Inventors: Carol M. Troy [US], Ying Y. Jean [US].
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Patent 2024
Adult Alcaine Cell Death Clotrimazole Diabetes Mellitus Edema Fluorescein Fluorescein Angiography Inflammation Injections, Intraperitoneal Ketamine Laser Ablation Mus Neoplasm Metastasis Optic Disk Photoreceptor Cells Pulse Rate Retina Retinal Edema Rose Bengal Tail Tomography, Optical Coherence Topical Anesthetics Vascular Endothelial Growth Factors Veins Veins, Central Retinal Vision Xylazine
4
Heartbeat Monitoring in Cluster Nodes
Not available on PMC !

Example 7

Based on the above examples, after the worker node successfully joins a cluster, the container image controller proxy component of the worker node sends an update request to the master node every 5 minutes. The update request content comprises the current node role (master node or worker node) of the node, the operating system, the kernel version of the operating system, and the node transmitting and updating time. Upon receiving this request, the master node updates the data corresponding to these fields in the database. At this time, the master node recursively inquires the update time for each node in the database every 10 minutes and then compares the update time with the current time. If the time difference is within 10 minutes, no operation will be performed. If the time difference is more than 10 minutes, the master node determines this node as a fault node and removes this node from the cluster. Based on the above embodiments, by setting the heartbeat detection program, it is determined whether a worker node operates normally or is disconnected abnormally.

US11868944B2. Container image management system for distributed clusters (2024-01-09). Nanjing University of Posts and Telecommunications [CN]. Inventors: Dengyin Zhang [CN], Junjiang Li [CN], Can Chen [CN], Chao Zhou [CN], Zijie Liu [CN].
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Patent 2024
Pulse Rate Workers
5
Spatiotemporal Relationship of Target Display Array
Not available on PMC !

EXAMPLE 1

In the example of FIG. 5, the generation rate V1 of the target pulse sequences is the same as the display rate V2 of the target display array, and the generation resolution R1 of the target pulse sequences is the same as the display resolution R2 of the target display array. The light-emitting state signal includes On and Off.

The ratio of the generation rate V1 to the display rate V2 is 1, and the ratio of the generation resolution R1 to the display resolution R2 is 1. Thus, the spatiotemporal relationship is determined as follows.

The target display array corresponds to one pulse plane of the input target pulse sequences, with each display unit corresponding to one pulse signal at one pulse position on the pulse plane. The display unit is, for example, a pixel unit.

The first preset threshold is 1. If the pulse signal is 1, then the accumulated pulse signal value is 1, and the display state information is lighting-up to control the corresponding display unit to light up. If the pulse signal is 0, then the accumulated pulse signal value is 0, and the display state information is lighting-off.

US11862053B2. Display method based on pulse signals, apparatus, electronic device and medium (2024-01-02). SPIKE VISION (BEIJING) TECHNOLOGY CO., LTD. [CN]. Inventors: Tiejun Huang [CN], Lei Ma [CN].
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Patent 2024
Medical Devices Pulse Rate

Top products related to «Pulse Rate»

1
Neon transfection system by Thermo Fisher Scientific
Sourced in United States, Germany, United Kingdom, Switzerland, France, Japan, China, Canada, Italy, Belgium, Luxembourg
The Neon Transfection System is a laboratory equipment designed for the efficient delivery of nucleic acids, such as DNA or RNA, into a variety of cell types. It utilizes electroporation technology to facilitate the transfer of these molecules across the cell membrane, enabling researchers to study gene expression, conduct functional assays, or modify cellular behavior.
2
Matlab by MathWorks
Sourced in United States, United Kingdom, Germany, Canada, Japan, Sweden, Austria, Morocco, Switzerland, Australia, Belgium, Italy, Netherlands, China, France, Denmark, Norway, Hungary, Malaysia, Israel, Finland, Spain
MATLAB is a high-performance programming language and numerical computing environment used for scientific and engineering calculations, data analysis, and visualization. It provides a comprehensive set of tools for solving complex mathematical and computational problems.
3
Topspin 3 by Bruker
Sourced in Germany, United States, Switzerland, United Kingdom, Italy, Spain, Canada, Australia
Topspin 3.2 is a software package developed by Bruker for the acquisition, processing, and analysis of nuclear magnetic resonance (NMR) data. It provides a comprehensive suite of tools for the management and interpretation of NMR spectra.
4
Avance 3 by Bruker
Sourced in Germany, United States, Switzerland, United Kingdom, France, Japan, Brazil
The Avance III is a high-performance NMR spectrometer by Bruker. It is designed for advanced nuclear magnetic resonance applications, providing reliable and accurate data acquisition and analysis capabilities.
5
Tim trio by Siemens
Sourced in Germany, United States, United Kingdom, China
The Tim Trio is a versatile laboratory equipment that serves as a temperature-controlled magnetic stirrer. It features three independent stirring positions, allowing simultaneous operation of multiple samples. The device maintains a consistent temperature range to ensure accurate and reliable results during experimental procedures.
6
32 channel head coil by Siemens
Sourced in Germany, United States, Australia, United Kingdom, Canada
The 32-channel head coil is a key component in magnetic resonance imaging (MRI) systems. It is designed to acquire high-quality images of the human head, enabling detailed visualization and analysis of brain structure and function.
7
Pclamp 10 by Molecular Devices
Sourced in United States, Germany, Canada, United Kingdom, China, Australia
PClamp 10 software is a data acquisition and analysis platform for electrophysiology research. It provides tools for recording, analyzing, and visualizing electrical signals from cells and tissues.
8
Opti mem by Thermo Fisher Scientific
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Opti-MEM is a cell culture medium designed to support the growth and maintenance of a variety of cell lines. It is a serum-reduced formulation that helps to reduce the amount of serum required for cell culture, while still providing the necessary nutrients and growth factors for cell proliferation.
9
Sphygmocor by AtCor Medical
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The SphygmoCor is a non-invasive medical device developed by AtCor Medical. Its core function is to measure and analyze the arterial pulse wave, providing insights into the cardiovascular system's health and function.
10
Discovery mr750 by GE Healthcare
Sourced in United States, Germany, United Kingdom, Netherlands
The Discovery MR750 is a magnetic resonance imaging (MRI) system developed by GE Healthcare. It is designed to provide high-quality imaging for a variety of clinical applications.

More about "Pulse Rate"

Cardiovascular Health and Pulse Rate Measurement: Unlocking Insights with PubCompare.ai Heart rate, also known as pulse rate, is a vital sign that provides crucial insights into an individual's cardiovascular health and overall physiological state.
This metric, typically measured in beats per minute (bpm), is influenced by various factors such as age, physical activity, emotions, and certain medical conditions.
Accurately measuring and monitoring pulse rate is essential for healthcare professionals when assessing a patient's condition, detecting abnormalities, and guiding appropriate medical interventions.
The PubCompare.ai platform can optimize pulse rate research by helping researchers locate the best protocols from literature, preprints, and patents, while using advanced comparisons to enhance reproducibility and accuracy.
Leveraging artificial intelligence, PubCompare.ai takes the guesswork out of your research and ensures you find the most reliable and effective protocols for your pulse rate studies.
Whether you're using Neon Transfection System, MATLAB, Topspin 3.2, Avance III, Tim Trio, 32-channel head coil, PClamp 10 software, Opti-MEM, or SphygmoCor, this platform can enhance your research efforts and help you make more informed decisions.
By accessing the latest literature, preprints, and patents, PubCompare.ai empowers researchers to stay at the forefront of pulse rate research, leveraging the most up-to-date and effective protocols.
Discover how this AI-driven platform can optimize your pulse rate studies and unlock valuable insights into cardiovascular health and overall physiological state.
OtherTerms: Heart rate, cardiovascular health, beats per minute, vital sign, medical condition, reproducibility, accuracy, Neon Transfection System, MATLAB, Topspin 3.2, Avance III, Tim Trio, 32-channel head coil, PClamp 10 software, Opti-MEM, SphygmoCor, Discovery MR750