Temperature is one of the most important factors that affects our daily lives. Everyone can recognize the arrival of spring by feeling the warmth in the air. Every chef pays attention to the temperature of a frying pan and an oven. In science, all phenomena, for example, chemical reactions or color of a star, are influenced by temperature. Therefore methods for measuring temperature remain in vogue. Until now, various types of thermometers have been developed, such as liquid-filled bulbs and stems (alcohol and mercury thermometers), bimetal strips, metallic resistors, thermistors, thermoelectric devices (thermocouples), and infrared radiation detectors (thermography) (1).A molecule that responds to heat and sends the information about temperature in the form of a light signal (e.g., fluorescence) is called a luminescent molecular thermometer (LMT). Such a "smart" molecule is able to function as a molecular-level thermometer (2, 3) in the scientific world. LMTs have a great advantage over other thermometers in measuring temperatures in a small space (with dimensions of < 10 ᎑3 m), since the fluorescence detection is highly sensitive and enables us to observe even one molecule (with a size of ∼10 ᎑9 m) (4). To measure two-or three-dimensional temperature distribution in space and to obtain the time sequence of temperature in a dewdrop, a living cell, a microfluidic channel, or a microreactor are a few of the goals in the application of LMTs. All of these places are too small for macroscopic thermometers but large enough to accommodate the smart molecular reporter.Thermally-driven Boltzmann-type distribution between two competing or equilibrating states is a useful model to rationalize most observations with luminescent molecular thermometers. If the two states show a difference in fluorescence quantum yield (Φ f ) (or fluorescence intensity), fluorescence lifetime (τ f ), or maximum emission wavelength (λ em ), the molecule can be used as a LMT. In this article, LMTs are classified into nine categories based on the spatial relationship between two competing or equilibrating states as shown in Table