E ﬀ ect of Warm Rolling Temperature on the Microstructure and Texture of Microcarbon Dual-Phase (DP) Steel

: The e ﬀ ect of warm rolling temperature on microstructure and texture of microcarbon dual-phase (DP) steel was investigated through scanning electron microscopy (SEM), electron backscatter di ﬀ raction (EBSD), and transmission electron microscopy (TEM). The results showed that with the increase of rolling temperature, the density and thickness of the deformation band ﬁrst increased and then decreased. Ferrite and ﬁne martensite were observed in the annealed sheet, and the ferrite had a much more homogeneous distribution in the sample rolled at 450 ◦ C. During warm rolling, the ferrite developed a dominant γ -ﬁber and a weak α -texture. During the annealing of the rolled sheet, the intensity of the γ -ﬁber was increased and a weak {001} < 100 > texture developed in the sample rolled at room temperature. An increase in the rolling temperature generated an initial decrease and subsequent increase in the strength of the unfavorable {001} < 110 > texture in the annealed sheet. In addition, the strength reached a maximum at 550 ◦ C due to an increase in the dissolved carbon in the matrix, which was result of carbide dissolution. By contrast, the intensity of the γ -ﬁber remained relatively higher and was deemed the weaker {001} < 110 > component in the annealed sheet rolled at 450 ◦ C. Therefore, a larger texture factor ( f γ -ﬁber / f ( α -ﬁber + λ -ﬁber ) ) can be produced under this process.


Introduction
Warm rolling technology is an effective method is used to improve the strength and deep-drawing properties of advanced high-strength steel (AHSS). In general, the tensile strength of interstitial free (IF) and bake-hardenable (BH) steel hardly exceeds 500 MPa because of the single ferrite matrix [1,2]. Ordinary high-strength or ultra-high-strength steels, such as dual-phase (DP) and transformation-induced plasticity (TRIP) steel, generate poor deep drawing properties and R-values that generally do not exceed 1.2 due to the abundance of C in solid solution in the matrix [3]. Due to the influence of the C atoms in the solid solution, development of the deep drawing texture (mainly consisting of γ-fiber) in microcarbon steel is not as complete as that in ultra-low carbon steel. Han et al. [4] presented a method to control the amount of C in the solid matrix solution via the low-temperature precipitation and high-temperature dissolution of the precipitates with chrome (Cr) and molybdenum (Mo). Wang et al. [5] found that the intensity of {001}<110> was significantly reduced by fixing the amount of C in the solid solution of Cr-Mo DP steel. Barnett [6] and Jonas [7] observed a very favorable in-grain shear band for the formation of γ-fiber in IF steels or low carbon (LC) steels, which is conducive for the development of the deep drawing texture. However, the low-temperature Metals 2020, 10, 566 2 of 14 deformation test results indicated the presence of very few shear bands and negative strain rate sensitivity (m) in the LC steel [8], resulting in the generation of dynamic strain aging (DSA) behavior. Many reports indicated the abundance of DSA behavior in LC steel at lower rolling temperatures, which inhibits the formation of shear bands and worsens the deep drawing texture [9,10]. Therefore, it is necessary to avoid or delay the DSA temperature region during the warm rolling of LC steel. Mohammad et al. [11] found that the addition of microalloying elements, such as Cr, can delay the DSA behavior. In addition, the in-grain shear band can also be generated during warm rolling at low temperatures. Cuddy and Leslie [12] reported similar conclusions, wherein the DSA behavior can be inhibited the C-Cr atom pair as well as the successful generation of shear bands after warm rolling.
Cr can increase the shear band contents, inhibit DSA behavior by forming large-sized precipitates, and improve tensile properties [13]. In addition, the present work also added Nb in the tested steel with the aim of fixing the C component in the solid solution. Nb has a strong affinity to C, allowing C atom pinning in the solid solution by forming precipitates and promoting favorable texture formation, including <111>//ND({111}//normal direction) fiber and {554}<225> component [14]. Hoseini and Anijdan [15] reported that Nb can intensify the {111} texture, particularly the {111}<112> component following 400 • C rolling. In addition, the NbC precipitates were reportedly able to strengthen the matrix [16].
The present study reported the effect of the warm rolling temperature on the microstructure and texture of the C-Cr-Nb DP steel during warm rolling and annealing. The main focus was the influence of the rolling temperature on the γ-fiber texture and α-fiber texture given that the former is favorable to deep drawabilities. Meanwhile, the evolution of the microstructure and texture was investigated and the causes of the texture formation and disappearance were further analyzed by scanning electron microscopy (SEM), electron backscatter diffraction (EBSD), and transmission electron microscopy (TEM). The results of this study provide the theoretical and parametric support for the warm rolling design process of microcarbon DP steel. Table 1 presents the chemical compositions of the experimental steel, in which rare earth (RE) elements were employed to purify the molten steel [17]. The tested steel was smelted in a 25 kg vacuum induction melting furnace and forged into a stock with dimensions of 90 mm × 60 mm × 30 mm.  Figure 1 presents a schematic illustration of the manufacture process. The forged billet was heated and soaked at 1200 • C for 2 h. The specimens were then hot-rolled to 5 mm at a finishing temperature of 870 • C and cooled at 700 • C held for 1.5 h to simulate the coiling process. The hot-rolled specimens were heated to a rolling temperature (250 • C to 550 • C, interval: 100 • C) that was maintained for 30 min, fed into the roll mill to generate 2-mm-thick specimen under a single pass, and finally quenched in water. Subsequently, the annealing process was performed on the bright annealing furnace (Type: SK-10-13H, Beijing Yanbei Jianxing Boiler Industry Co.,Ltd., Beijing, China), to which the specimens were heated to 830 • C (heating rate: 8 • C S −1 ; AC1: 780 • C; and AC3: 900 • C, which was calculated using JMatPro 9.0 software, England) and held for 120 s under nitrogen gas and then rapidly cooled to room temperature using cool water.

Experimental Methods
The microstructure and texture observed in RD-ND (rolling direction and normal direction) plane using scanning electron microscopy (SEM, Carl Zeiss AG, Jena, Germany) coupled with electron backscattered diffraction (EBSD; OXFORD Corporation, Oxford Instrument Technology Co., Ltd., Shanghai, China) with Channel 5.0 HKL software (Tango, Mambo and Salsa model, ϕ2 = 45 • cross-section, OXFORD). The EBSD-related experimental parameters are detailed as follows: a working voltage of 20 kV, a working distance of 15 mm, and a step size between 0.28 µm and 0.36 µm. In all of the descriptions, the α-, γ-, and λ-fibers were equivalent to <110>//RD, <111>//ND, and <100>//RD. TEM specimen preparation was applied as follows: thin slices were cut from a 2-mm thick sheet with wire cutter and ground to 50 µm and then punched into a circle with a diameter of 3 mm; the 5% perchlorate alcohol solution was used for electropolishing; and the voltage was set between 30 V and 40 V. The SEM and EBSD specimens were applied by mechanical polishing and electropolishing.
Metals 2020, 10, x FOR PEER REVIEW 3 of 14 45°cross-section, OXFORD). The EBSD-related experimental parameters are detailed as follows: a working voltage of 20 kV, a working distance of 15 mm, and a step size between 0.28 μm and 0.36 μm. In all of the descriptions, the α-, γ-, and -fibers were equivalent to <110>//RD, <111>//ND, and <100>//RD. TEM specimen preparation was applied as follows: thin slices were cut from a 2-mm thick sheet with wire cutter and ground to 50 μm and then punched into a circle with a diameter of 3 mm; the 5% perchlorate alcohol solution was used for electropolishing; and the voltage was set between 30 V and 40 V. The SEM and EBSD specimens were applied by mechanical polishing and electropolishing.

Microstructure Feature
The warm rolling temperature significantly influences the thickness and distribution of the deformation band [18]. Figure 2a presents the warm-rolled microstructure composed of a small pearlite block (red dotted line frame) in the matrix. Figure 2b,c present the grain boundary carbides and pearlite fiber band, respectively, that may have been caused by the fragmentation of pearlite in the hot-rolling sheet after room temperature rolling. The ferrite elongated along the RD-direction (Figure 2c-f). The elongated pearlite bands and a wide ferrite deformation band thickness were observed at 250 °C (Figure 2c). At 350 °C, the deformation band thickness was similar to that at 250 °C, though a significantly reduced deformation pearlite band was observed. A more refined deformation band was detected at a temperature of 450 °C and at the highest density (proportion of the deformation bands area in the total field), during which the large size carbides disappeared to present a more uniform deformation. The deformation degree dramatically decreased and the band thickness significantly widened at 550 °C possibly due to the dynamic recovery at this temperature.

Microstructure Feature
The warm rolling temperature significantly influences the thickness and distribution of the deformation band [18]. Figure 2a presents the warm-rolled microstructure composed of a small pearlite block (red dotted line frame) in the matrix. Figure 2b,c present the grain boundary carbides and pearlite fiber band, respectively, that may have been caused by the fragmentation of pearlite in the hot-rolling sheet after room temperature rolling. The ferrite elongated along the RD-direction (Figure 2c-f). The elongated pearlite bands and a wide ferrite deformation band thickness were observed at 250 • C (Figure 2c). At 350 • C, the deformation band thickness was similar to that at 250 • C, though a significantly reduced deformation pearlite band was observed. A more refined deformation band was detected at a temperature of 450 • C and at the highest density (proportion of the deformation bands area in the total field), during which the large size carbides disappeared to present a more uniform deformation. The deformation degree dramatically decreased and the band thickness significantly widened at 550 • C possibly due to the dynamic recovery at this temperature.  Figure 3 presents the annealing microstructure, which is composed of ferrite and martensite. The deformed ferrite grain has a finishing recrystallization that tended to be equiaxed. The martensite grain size was larger and the distribution was uneven compared to the specimen that was rolled at room temperature. However, the specimen below 350 °C was not completely recrystallized given the presence of some thin deformed bands after annealing (red dotted line in Figure 3b,c), which may be a result of the stored energy, wherein obvious martensite aggregation was observed at room temperature and at 350°C (red dotted box in Figure 3a,c). The deformed band disappeared, a relatively clear grain boundary was observed when the rolling temperature was increased to 450 °C ( Figure 3e). In addition, Figure 3f indicates the presence of a martensite island in the ferrite grain boundary. The ferrite grain size and martensite distribution at 550 °C were less uniform than at 450 °C.   Figure 3 presents the annealing microstructure, which is composed of ferrite and martensite. The deformed ferrite grain has a finishing recrystallization that tended to be equiaxed. The martensite grain size was larger and the distribution was uneven compared to the specimen that was rolled at room temperature. However, the specimen below 350 • C was not completely recrystallized given the presence of some thin deformed bands after annealing (red dotted line in Figure 3b,c), which may be a result of the stored energy, wherein obvious martensite aggregation was observed at room temperature and at 350 • C (red dotted box in Figure 3a,c). The deformed band disappeared, a relatively clear grain boundary was observed when the rolling temperature was increased to 450 • C ( Figure 3e). In addition, Figure 3f indicates the presence of a martensite island in the ferrite grain boundary. The ferrite grain size and martensite distribution at 550 • C were less uniform than at 450 • C.  Figure 3 presents the annealing microstructure, which is composed of ferrite and martensite. The deformed ferrite grain has a finishing recrystallization that tended to be equiaxed. The martensite grain size was larger and the distribution was uneven compared to the specimen that was rolled at room temperature. However, the specimen below 350 °C was not completely recrystallized given the presence of some thin deformed bands after annealing (red dotted line in Figure 3b,c), which may be a result of the stored energy, wherein obvious martensite aggregation was observed at room temperature and at 350°C (red dotted box in Figure 3a,c). The deformed band disappeared, a relatively clear grain boundary was observed when the rolling temperature was increased to 450 °C ( Figure 3e). In addition, Figure 3f indicates the presence of a martensite island in the ferrite grain boundary. The ferrite grain size and martensite distribution at 550 °C were less uniform than at 450 °C.    Figure 4f presents the volume fraction of several typical texture orientations and texture factors (f γ-fiber /f (α-fiber+λ-fiber) ) [19], wherein the volume fraction of the {111}//ND texture reached a peak at 450 • C, which was conducive to the formation of the γ-fiber. In comparison, a mere 22% of the γ-fiber was observed at 550 • C (Figure 4f). The content of the <100>//ND texture was less than that of the {111}//ND texture, which was mainly concentrated on the {001}<110> texture at both 350 • C and 450 • C. The 450 • C and 550 • C specimens presented the lowest and highest α-fiber contents, respectively. In addition, the 450 • C specimen exhibited the largest texture factor, as shown in Figure 4f for {111}/{110}+{100}. The rolling temperature greatly affected the γ-fiber and {001}<110> content. Warm rolling was highly unlikely to produce {001}<100> as compared to rolling at room temperature. {001}<110> was more easily produced between 250 • C and 450 • C. In addition, warm rolling at 550 • C was more prone to generating α-fiber.  Figure 4f presents the volume fraction of several typical texture orientations and texture factors (fγ-fiber/f(α-fiber + -fiber)) [19], wherein the volume fraction of the {111}//ND texture reached a peak at 450°C, which was conducive to the formation of the γ-fiber. In comparison, a mere 22% of the γ-fiber was observed at 550 °C (Figure 4f). The content of the <100>//ND texture was less than that of the {111}//ND texture, which was mainly concentrated on the {001}<110> texture at both 350 °C and 450 °C. The 450 °C and 550° C specimens presented the lowest and highest α-fiber contents, respectively. In addition, the 450 °C specimen exhibited the largest texture factor, as shown in Figure 4f for {111}/{110}+{100}. The rolling temperature greatly affected the γ-fiber and {001}<110> content. Warm rolling was highly unlikely to produce {001}<100> as compared to rolling at room temperature. {001}<110> was more easily produced between 250 °C and 450 °C. In addition, warm rolling at 550 °C was more prone to generating α-fiber.   Figure 5b shows the γ-fiber density of the warm-rolled sheet. The total density line showed high intensity at 450 °C,        Figure 7 presents the α-and γ-fiber density calculation results. The density of the unfavorable texture was higher in the adjacent {001}<110> and {221}<110> components at room temperature. At 250 °C, the α-recrystallization texture was concentrated between {001}<110> and {111}<110>. Weak α-recrystallization texture was observed at 350 °C, whereas higher density was observed in the adjacent {112}<110> content at 550 °C, indicating relatively low γ-recrystallization texture that was still not conducive to the deep drawing properties (Figure 7b). Nevertheless, at 450 °C, the specimen exhibited strong γ-recrystallization texture. In addition, density of {112}<110> orientation was two-fold higher than that of the {111}<110> orientation in Figure 6d and Figure 7b due to the texture inheritance.  At 250 • C, the α-recrystallization texture was concentrated between {001}<110> and {111}<110>. Weak α-recrystallization texture was observed at 350 • C, whereas higher density was observed in the adjacent {112}<110> content at 550 • C, indicating relatively low γ-recrystallization texture that was still not conducive to the deep drawing properties (Figure 7b). Nevertheless, at 450 • C, the specimen exhibited strong γ-recrystallization texture. In addition, density of {112}<110> orientation was two-fold higher than that of the {111}<110> orientation in Figures 6d and 7b due to the texture inheritance. The texture evolution beginning from the warm rolling to annealing was further analyzed. Figure 8 lists the eight typical textures that were analyzed, wherein the intensity of the γ-fiber and {554}<225> component increased with temperature from 250 °C to 450 °C. The textures slightly weakened after annealing and reached a relative balance at 450 °C. Although the γ-fiber content increased after annealing the 550 °C specimen, it was still weak possibly due to the dynamic recovery. The α-deformation texture content first decreased and then increased across the temperature range of room temperature to 550 °C, during which the lowest content was observed at 450 °C, at which time all of the content decreased after annealing. The γ-fiber only increased or remained stable after annealing when the {223}<110> and {112}<110> contents exceeded 20% in the warm-rolled sheet, such that the γ-fiber increased after annealing. The {001}<110> density of the -fiber significantly decreased after annealing at 350 °C as compared to annealing at room temperature or at 250 °C. Warm rolling was able to greatly reduce the influence of {001}<100> and {001}<110>. In summary, rolling within the temperature range of 250 °C to 450 °C exhibited significantly higher texture factors as compared to other temperatures (Table 2). Moreover, maximum texture factor strength was observed at 450 °C for both the warm-rolled and annealed specimen, indicating optimized deep drawing properties, as indicated by the results presented in Figure 4f and Figure 6f   The texture evolution beginning from the warm rolling to annealing was further analyzed. Figure 8 lists the eight typical textures that were analyzed, wherein the intensity of the γ-fiber and {554}<225> component increased with temperature from 250 • C to 450 • C. The textures slightly weakened after annealing and reached a relative balance at 450 • C. Although the γ-fiber content increased after annealing the 550 • C specimen, it was still weak possibly due to the dynamic recovery. The α-deformation texture content first decreased and then increased across the temperature range of room temperature to 550 • C, during which the lowest content was observed at 450 • C, at which time all of the content decreased after annealing. The γ-fiber only increased or remained stable after annealing when the {223}<110> and {112}<110> contents exceeded 20% in the warm-rolled sheet, such that the γ-fiber increased after annealing. The {001}<110> density of the λ-fiber significantly decreased after annealing at 350 • C as compared to annealing at room temperature or at 250 • C. Warm rolling was able to greatly reduce the influence of {001}<100> and {001}<110>. In summary, rolling within the temperature range of 250 • C to 450 • C exhibited significantly higher texture factors as compared to other temperatures (Table 2). Moreover, maximum texture factor strength was observed at 450 • C for both the warm-rolled and annealed specimen, indicating optimized deep drawing properties, as indicated by the results presented in Figures 4f and 6f (green line).

Discussion
Generally speaking, warm rolling in low carbon steel is presented when the rolling temperature is lower than the ferrite recrystallization temperature but higher than room temperature rolling. [20]. Compared with austenitic rolling, warm rolling avoids the effect of phase transition, thus resulting in more uniform final steel mechanical properties. In the process of warm rolling, the deformation band is an important microstructure. The influence of the temperature on the deformation bands is discussed in this experiment, as gradual form is observed with the rise in rolling temperature due to inhomogeneity deformation and can be related to the local plastic instability during the rolling process [21]. Therefore, the deformation band was not easily generated at room temperature as well as under an excessive temperature (such as 550 °C). The dislocation density decreased, the ferrite deformation band widened, and the deformation degree decreased due to dynamic recovery at a rolling temperature of 550 °C. Uniform and narrow deformation bands were formed in specimen at 450 °C rolling, which provided more nucleation points for martensitic transformation in quenching. In addition, evenly distributed ferrite grain as well as a small and uniformly distributed martensitic phase was also observed. At 250 °C and 350 °C, the uneven deformation band and the incomplete

Discussion
Generally speaking, warm rolling in low carbon steel is presented when the rolling temperature is lower than the ferrite recrystallization temperature but higher than room temperature rolling [20]. Compared with austenitic rolling, warm rolling avoids the effect of phase transition, thus resulting in more uniform final steel mechanical properties. In the process of warm rolling, the deformation band is an important microstructure. The influence of the temperature on the deformation bands is discussed in this experiment, as gradual form is observed with the rise in rolling temperature due to inhomogeneity deformation and can be related to the local plastic instability during the rolling process [21]. Therefore, the deformation band was not easily generated at room temperature as well as under an excessive temperature (such as 550 • C). The dislocation density decreased, the ferrite deformation band widened, and the deformation degree decreased due to dynamic recovery at a rolling temperature of 550 • C. Uniform and narrow deformation bands were formed in specimen at 450 • C rolling, which provided more nucleation points for martensitic transformation in quenching. In addition, evenly distributed ferrite grain as well as a small and uniformly distributed martensitic phase was also observed. At 250 • C and 350 • C, the uneven deformation band and the incomplete broken pearlite group resulted in the uneven distribution and a larger martensite grain during the annealing process.
The α-deformation texture was easily formed during warm rolling. In addition, warm rolling was more likely to produce {001}<110> mainly due to the strongest uniform deformation band at 450 • C. Figure 9a shows the orientation distribution diagram at 350 • C. Figure 9a presents the mildly deformed <111>//ND grains (blue color), and Figure 9b further indicates the deformed grain belonging to the {111}<112> orientation (purple color). In addition, severely deformed and elongated grains that were mainly representative of the α-orientation grains (Figure 9c) were observed in the green color area. However, the grain will not stop rotating immediately when the rolling temperature was too high (550 • C). That is, the grain continue to rotate to reach the stable state, such that the experimental results showed that the stable orientation was close to the <110>//RD orientation.
Metals 2020, 10, x FOR PEER REVIEW 10 of 14 broken pearlite group resulted in the uneven distribution and a larger martensite grain during the annealing process. The α-deformation texture was easily formed during warm rolling. In addition, warm rolling was more likely to produce {001}<110> mainly due to the strongest uniform deformation band at 450 °C. Figure 9a shows the orientation distribution diagram at 350 °C. Figure 9a presents the mildly deformed <111>//ND grains (blue color), and Figure 9b further indicates the deformed grain belonging to the {111}<112> orientation (purple color). In addition, severely deformed and elongated grains that were mainly representative of the α-orientation grains (Figure 9c) were observed in the green color area. However, the grain will not stop rotating immediately when the rolling temperature was too high (550 °C). That is, the grain continue to rotate to reach the stable state, such that the experimental results showed that the stable orientation was close to the <110>//RD orientation. Deformation bands were formed by the interactions between the dislocations as well as between the precipitates and dislocations, thereby resulting in crystal bending [22]. According to Figure 10a, the dislocation density increased on the Cr-rich carbide region at low temperatures. In addition, the interactions between the dislocations also increased (Figure 10b), thereby resulting in local stress concentration, inhomogeneity deformation, and difficult grain rotation. A transition band was formed between the two deformation bands. The transition band between two {111}<112> grains easily formed α-texture (Figure 9a,b; white and black line). Precipitate interaction with the dislocation was more likely to occur at higher temperatures when the atomic diffusion rate was equal to the slip rate of the dislocation [23] (Figure 10b). A rolling temperature of 450 °C induced the precipitates to undergo dislocation pinning as well as resulted in plane slip dislocations, thus promoting deformation band production, which resulted in increased {001}<110> content [24]. The Deformation bands were formed by the interactions between the dislocations as well as between the precipitates and dislocations, thereby resulting in crystal bending [22]. According to Figure 10a, the dislocation density increased on the Cr-rich carbide region at low temperatures. In addition, the interactions between the dislocations also increased (Figure 10b), thereby resulting in local stress concentration, inhomogeneity deformation, and difficult grain rotation. A transition band was formed between the two deformation bands. The transition band between two {111}<112> grains easily formed α-texture (Figure 9a,b; white and black line). Precipitate interaction with the dislocation was more likely to occur at higher temperatures when the atomic diffusion rate was equal to the slip rate of the dislocation [23] (Figure 10b). A rolling temperature of 450 • C induced the precipitates to undergo dislocation pinning as well as resulted in plane slip dislocations, thus promoting deformation band production, which resulted in increased {001}<110> content [24]. The cellular dislocation substructure was observed and certain grains exhibited dynamic recovery (Figure 10c) as the rolling temperature continued to increase to 550 • C. In addition, unfavorable C atomic content was observed in the matrix due to the development of deep drawn texture, which served as an effective mean to fixing C by forming carbides. However, no M23C6 carbides were found in the TEM photographs. A similar conclusion was produced based on the JMatPro software calculations (Figure 10d), which showed no M23C6 precipitates at 550 • C, indicating that the C content of matrix was higher than that at other temperatures, which was not conducive to the development of the deep draw texture. Dynamic recovery was observed at 550 • C, and the dislocation density was sharply released, indicating the likely formation of the α-fiber [25].
Metals 2020, 10, x FOR PEER REVIEW 11 of 14 cellular dislocation substructure was observed and certain grains exhibited dynamic recovery (Figure 10c) as the rolling temperature continued to increase to 550 °C. In addition, unfavorable C atomic content was observed in the matrix due to the development of deep drawn texture, which served as an effective mean to fixing C by forming carbides. However, no M23C6 carbides were found in the TEM photographs. A similar conclusion was produced based on the JMatPro software calculations (Figure 10d), which showed no M23C6 precipitates at 550 °C , indicating that the C content of matrix was higher than that at other temperatures, which was not conducive to the development of the deep draw texture. Dynamic recovery was observed at 550 °C, and the dislocation density was sharply released, indicating the likely formation of the α-fiber [25]. The grain with γ orientation gradually consumed the grain with α-orientation during annealing because the former has relatively higher deformation stored energy. Warm rolling technology promoted the formation of the γ-deformation texture according to an analysis on the deformation texture, thus promoting the production of the γ-recrystallization texture, especially for the specimen at 450 °C. However, the recrystallization texture was mainly inherited from the hot-rolled sheet. In The grain with γ orientation gradually consumed the grain with α-orientation during annealing because the former has relatively higher deformation stored energy. Warm rolling technology promoted the formation of the γ-deformation texture according to an analysis on the deformation texture, thus promoting the production of the γ-recrystallization texture, especially for the specimen at 450 • C. However, the recrystallization texture was mainly inherited from the hot-rolled sheet. In addition, it was impossible to form recrystallization texture at room temperature rolling. Figures 4 and 7 present a small difference between the main texture types under warm rolling and annealing conditions, especially for the γ-fiber. These difference were due to the transformation between {111}<112> and {111}<110> during annealing [26,27]. However, in the annealing, the deformed {111}<112> and {111}<110> component will be converted to recrystallized {111}<110> and {111}<112> component correspondingly, indicating an insignificant difference between the two components [28].
The grain orientation and size distribution of the annealed specimens at 450 • C and 550 • C were studied to further explore the effect of the warm rolling temperature on the recrystallization texture. The results indicated that the grain orientation of <111>//ND dominated at an annealing of 450 • C. However, many small grains were observed at 550 • C even after the complete recrystallization. In addition, these grains was mostly likely followed non-<111>//ND grain orientation (Figure 11b; dotted circle). According to Figure 11c, the specimen at 550 • C exhibited a greater dispersion coefficient (0.74513) compared to the specimen at 450 • C (0.68894). A normal distribution of the grain size and a relatively uniform ferrite and martensite distribution were observed at 450 • C, indicating mixed crystal microstructure production at a rolling temperature of 550 • C after annealing.  [28]. The grain orientation and size distribution of the annealed specimens at 450 °C and 550 °C were studied to further explore the effect of the warm rolling temperature on the recrystallization texture. The results indicated that the grain orientation of <111>//ND dominated at an annealing of 450 °C. However, many small grains were observed at 550 °C even after the complete recrystallization. In addition, these grains was mostly likely followed non-<111>//ND grain orientation (Figure 11b; dotted circle). According to Figure 11c, the specimen at 550 °C exhibited a greater dispersion coefficient (0.74513) compared to the specimen at 450 °C (0.68894). A normal distribution of the grain size and a relatively uniform ferrite and martensite distribution were observed at 450 °C , indicating mixed crystal microstructure production at a rolling temperature of 550 °C after annealing.

Conclusions
(1) The warm rolling of C-Cr-Nb steel was more conducive to the formation of a deformation band as compared to room-rolling. Deformation bands with higher densities and narrower thicknesses were observed in the sample rolled at 450 °C. The annealed sheet had a ferrite and fine martensite microstructure that annealed at the inter-critical region. The ferrite matrix

Conclusions
(1) The warm rolling of C-Cr-Nb steel was more conducive to the formation of a deformation band as compared to room-rolling. Deformation bands with higher densities and narrower thicknesses were observed in the sample rolled at 450 • C. The annealed sheet had a ferrite and fine martensite microstructure that annealed at the inter-critical region. The ferrite matrix exhibited a much more homogeneous distribution after annealing in the sample rolled at 450 • C as compared to other rolling temperature.