The magnetism for the electrochemically prepared Li
xCoO
2 samples with 0.1
x![less-than-or-equals, slant less-than-or-equals, slant](http://www.sciencedirect.com/scidirimg/entities/2a7d.gif)
1 was investigated by muon-spin rotation/relaxation (μSR) and susceptibility (
χ) measurements. The
χ(
T) curves with
H=10 kOe, which correspond to the change in macroscopic magnetism, are almost
T-independent down to
![not, vert, similar not, vert, similar](http://www.sciencedirect.com/scidirimg/entities/223c.gif)
50 K for the
x![less-than-or-equals, slant less-than-or-equals, slant](http://www.sciencedirect.com/scidirimg/entities/2a7d.gif)
0.44 samples, suggesting that the samples in this
x range are Pauli-paramagnetic. For the samples with 0.49
x![less-than-or-equals, slant less-than-or-equals, slant](http://www.sciencedirect.com/scidirimg/entities/2a7d.gif)
3/4, a cusp is, however, observed around 170 K in their
χ(
T) curve. Since there are no anomalies in the μSR parameters around 170 K and μSR is sensitive to local magnetic nature, the cusp is most unlikely due to a magnetic transition, but either a spin state transition or a structural phase transition. Furthermore, zero-field μSR time spectra for all the samples mainly show a slow Kubo–Toyabe behavior, indicating that muon spin is mainly depolarized by randomly oriented nuclear moments of
7Li and
59Co. Hence, it was clarified that all the Li
xCoO
2 samples with
x<1 are paramagnetic even at 1.8 K, in contrast to Na
xCoO
2 and K
xCoO
2.