Page 16 - Read Online
P. 16

Su et al. J Cancer Metastasis Treat 2020;6:19 I  http://dx.doi.org/10.20517/2394-4722.2020.48                                Page 11 of 21


                  A                                             B



















                                     C                                                              D















                             E













               Figure 5. The Z-lab device can be connected to multiple types of devices such as cell phones, tablets, laptops, and desktop computers
               (A); the Z-Lab platform consists of three parts: a plastic cartridge, an electrical interface connecting the electrodes from GMR chip to
               the circuit board, and a handheld device (B); the layout of the GMR sensors (C); schematic illustration of the magnetic immunoassays
               on the sensor surface (D); real-time binding curve readout from Z-lab device (E) [50]  (reprinted with permission from American Chemical
               Society). GMR: giant magnetoresistance


               of the GMR-CMOS interface in addition to noise removal circuit for such handheld device, thereby
               immensely contributing to the sensitivity of the handheld device [79,80] .


               NMR
               Origin of NMR signal
                                                                                   1
                                                                                      15
                                                                                              31
                                                                                          17
               Elements that contain an odd number of protons and/or neutrons, such as  H,  N,  O,  P, etc., show
               intrinsic nonzero nuclear spins that give rise to small magnetic moments which can be observed by the
               NMR spectroscopy. Under a strong constant magnetic field B , the magnetic moments are in equilibrium
                                                                    0
               states, i.e., aligned either with or against the field denoted as M  in Figure 6A [81,82] . A perturbation of the
                                                                      0
               nuclear spins from equilibrium will occur when a weak oscillating magnetic field [referred to as radio
               frequency (rf) pulse] is applied whose frequency closely matches the nuclei’s intrinsic Larmor frequency.
   11   12   13   14   15   16   17   18   19   20   21