UCNPs are usually obtained from rare earth fluorides, oxides, oxyhalides and other matrix materials by doping trivalent activator ions and sensitizer ions. The Er
3+, Tm
3+ and Ho
3+ of lanthanide ions have abundant ladder-like energy levels, which have long lifetimes due to the effective shielding of the 5s
25p
6 electron shell. The energy difference between adjacent energy levels is very close, which is conducive to the continuous absorption of excitation photons, so they are easy to produce up-conversion luminescence phenomenon, and are the most widely used activator ions at present (Fig. 1. Ⅵ Energy Level Diagram). In order to improve the light absorption ability and luminescence efficiency of UCNPs, it is necessary to dope high concentration of sensitizer ions. An ideal sensitizer ion needs to meet two basic requirements: (1) the sensitizer ion has a large absorption cross section at the pump wavelength; (2) The energy difference between the excited state and the ground state of the sensitizer ion is very close to the energy difference between adjacent energy levels of the activator ion. Common sensitizer ions mainly include Yb
3+ and Nd
3+,In which the Yb
3+ contains only two energy levels that differ by 10
4cm
-1 (i.e., the ground state
2 and excited state
2 ),Its characteristic absorption wavelength is well matched with the most commonly used 980 nm pump laser.And its excited state
2 is consistent with the metastable excited state energies of Er
3+(
4I
11/2), Tm
3+(
3H
5) and Ho
3+(
5I
6.Therefore, the Yb
3+ can efficiently transfer the excitation energy to the most commonly used sensitizers in Er
3+, UTm
3+ and Ho
3+ upconversion luminescence. Nd
3+ is another excellent sensitizer ion, which has a strong ability to absorb 808 nm excitation light. The excited Nd
3+ can efficiently transfer the pump energy to the Yb
3+, and then the Yb
3+ transfers the energy to the activator ion to produce upconversion luminescence. Upconversion luminescence is one of the most important physical and chemical properties of UCNPs, which includes two aspects of luminescence, namely intensity and color. There are many factors affecting the upconversion luminescence properties, such as the type and concentration of dopant ions, host lattice, particle size and so on, among which adjusting the type and content of dopant ions is a very efficient and convenient method. For the upconversion luminescence system co-doped with Yb
3+-Ln
3+(Ln
3+=Er
3+, Tm
3+ and Ho
3+,There is an optimal doping concentration (C
opt) for both sensitizer Yb
3+ and activator Ln
3+. When the doping concentration of the Yb
3+ is increased from 0 to C
opt, the energy absorption efficiency is gradually improved, so that the luminescent intensity is increased; When the doping concentration of the Yb
3+ is further increased, the Ln
3+ will return most of the excitation energy to the Yb
3+ (that is, energy return) and weaken the upconversion luminescence. When the doping concentration of Ln
3+ increases from 0 to C
opt, the number of luminescence centers increases correspondingly, and the luminescence intensity naturally increases significantly. When the concentration is further increased to be higher than the C
opt, the strong interaction between adjacent Ln
3+ leads to the concentration quenching effect, and the luminescence intensity decreases significantly. Generally speaking, when the doping concentration of sensitizer Yb
3+ is 15% ~ 40%, the concentration of activator Er
3+ is 2%~6%,Tm
3+/Ho
3+, and the doping concentration is 0.1% ~ 1%, the upconversion luminescence intensity is optimal. The luminescent color can also be adjusted by changing the concentration of the doped ions, and when the contents of the Yb
3+ and the Ln
3+ are adjusted, the relative intensity of each emission peak of the Ln
3+ is changed, so that the modulation of the luminescent color is realized. In general, the system co-doped with Yb
3+-Er
3+ and Yb
3+-Ho
3+ mainly emits green light (Er
3+:
2H
11/2,
4S
3/2→
4I
15/2;Ho
3+:
5F
4,
5S
2→
5I
8). By properly increasing the concentration of Yb
3+ or Er
3+/Ho
3+, the emission intensity ratio of red light to green light increases, and the emission color changes to yellow or even red light. The Yb
3+-Tm
3+ co-doped system has two high-intensity emission peaks in the blue region, corresponding to the
1D
2→
3F
4(450 nm) and
1G
4→
3H
6(475 nm) transitions, and the energy level transition probability of the red emission is very low and is extremely difficult to improve, so the system always emits blue visible light. In addition, the construction of UCNPs with core-shell structure is another effective way to control the luminescent properties of materials. Due to the small size, the UCNPs core particles have a large specific surface area, and there are more surface defects and surface ligands that can induce fluorescence quenching, resulting in more non-radiative relaxation loss of activator ions near the surface, so the emission intensity is often low. In addition, for UCNPs, the low phonon energy mode is blocked by the phonon confinement effect, which reduces the energy transfer from the sensitizer ion to the activator ion, and also reduces the upconversion luminescence intensity. The luminescent intensity of UCNPs can be significantly enhanced by coating the core particles with shell materials with similar lattice constants, and the luminescent color of the materials can be easily modulated. The shell of UCNPs can be divided into three types: inert shell, sensitized shell and active shell. The inert shell is composed of an undoped matrix material and can greatly inhibit the fluorescence quenching effect caused by the surface defects of the core particles, the surface ligands and the high-energy vibration of solvents, thereby achieving the purpose of enhancing the luminous intensity of the core particles; The sensitization shell is composed of a matrix material doped with sensitizer ions, which not only has the function of an inert shell, but also can endow the UCNPs with more sensitizer ions to enhance the absorption capacity and the transmission efficiency of pump light,And the sensitizer ions in the shell layer are spatially isolated from the activator ions in the core particles, so that the energy backtransfer effect induced by high-concentration sensitizer doping is inhibited, and the luminescence enhancement effect is stronger; The active shell is obtained by doping the host material with activator ions, and generally, the activator ions in the shell layer are different from the activator in the core particle and can be up-conversion luminescence centers (Er
3+, Tm
3+, Ho
3+),It can also be commonly used down-conversion rare earth ions (Eu
3+, Tb
3+, Sm
3+, Dy
3+) and Mn
2+. The active shell can ensure the upconversion luminescence of all activator ions in the core-shell structure, thereby realizing the modulation of the luminescent color of the system and simultaneously improving the overall luminescent intensity
[34⇓⇓⇓⇓~39]. In view of the adjustable luminescence properties of lanthanide ions and the regularity of their changes, UCNPs meeting specific luminescence requirements can be designed and constructed under the guidance of upconversion luminescence mechanism.Novel luminescent properties such as multicolor orthogonal up-conversion and power density-dependent color conversion can be achieved, which can help to produce high-security luminescent labels that are difficult to counterfeit, thus providing advanced, sophisticated and complex fluorescent anti-counterfeiting technology.