An insulating bulk state is a prerequisite for the protection of topological edge states 1 . In quantum Hall systems, the thermal excitation of delocalized electrons is the main route to breaking bulk insulation 2 . In equilibrium, the only way to achieve a clear bulk gap is to use a high-quality crystal under high magnetic field at low temperature. However, bulk conduction could also be suppressed in a system driven out of equilibrium such that localized states in the Landau levels are selectively occupied. Here we report a transient suppression of bulk conduction induced by terahertz wave excitation between the Landau levels in a GaAs quantum Hall system. Strikingly, the Hall resistivity almost reaches the quantized value at a temperature where the exact quantization is normally disrupted by thermal fluctuations. The electron localization is realized by the long-range potential fluctuations, which are a unique and inherent feature of quantum Hall systems. Our results demonstrate a new means of e ecting dynamical control of topology by manipulating bulk conduction using light.The integer quantum Hall effect (IQHE) is a universal phenomenon observable in two-dimensional electron systems under high magnetic field (B). The Hall resistivity (ρ xy ) is quantized and the longitudinal resistivity (ρ xx ) becomes zero irrespective of the detailed properties of the host materials [2][3][4][5][6][7] . This universality has lead to a new physical concept of topological invariant that defines the quantized value of ρ xy (ref. 8). In systems with sample boundaries, edge metallic states appear according to the bulk/edge correspondence 9 and carry quantized Hall current. The edge states are protected by the bulk gap between the Landau levels (LLs), which prohibits the scattering between macroscopically separated edge states 10,11 . In realistic situations, we need to take into account the impurity and finite-temperature effect. The LLs are broadened with delocalized states in the centre, sandwiched by localized states induced by Anderson localization 12,13 (Fig. 1d). At finite temperatures, the delocalized states are broadened and thermally populated, which makes the bulk conductive 2,14 . As a result, the scattering between edge states is allowed and ρ xy (ρ xx ) is no longer quantized (zero).In this paper, we demonstrate a transient suppression of bulk conduction and a recovery of the quantized ρ xy by selectively populating the localized electronic states. A direct way to manipulate the electron distribution in LLs is inter-LL transition by resonant light absorption (typically in the terahertz frequency region). To verify this strategy for realizing light-induced IQHE, we performed transient Hall measurements on a quantum Hall system with a non-equilibrium electron distribution induced by picosecond terahertz pulse excitation. Previous research of this kind [15][16][17][18][19][20][21] was done in an ideal quantum Hall state and explained by the heating effect due to the nanosecond to microsecond terahertz pulses they empl...