Low-temperature Peak Research Articles

Structural, compositional and luminescence studies of Y2O3:Eu3+ nanophosphor synthesized by sol-gel method

Europium doped Yttrium oxide (Y2O3) nanophosphors with different doping concentrations were synthesized by simple and efficient sol-gel method. The structural, morphological and compositional study was carried out by using XRD, FE-SEM, TEM, EDS, XPS, etc. Results demonstrated that the material is highly crystalline with cubic (body centered) structure and the particles apparently are of spherical shape with particle size around ∼10–20 nm. EDS results show the presence of Eu-impurity evenly distributed. Optimization of luminescence properties of the material by varying the concentration and annealing temperature show maximum thermoluminescence (TL) sensitivity at 1600 °C for 10.0 M% of Eu, however, maximum photoluminescence (PL) intensity was achieved after annealing the nanophosphor at 1200 °C. It exhibits a strong red emission with a sharp peak at 612 nm under excitation with UV and visible light (λex = 260, 393, 466 nm). TL studies showed four peaks at 100, 117, 139, and 301 °C. However, the first peak fades completely in a day (apparently due to low peak temperature) but the other three peaks are quite stable. The TL response was found to be linear from 120 Gy to 1.0 kGy but becomes sub-linear later in the dose range 1.0–100 kGy.

Material Defects and Dark Currents in InGaAs/InP Avalanche Photodiode Devices

An In <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.53</sub> Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.47</sub> As/indium phosphide (InP) avalanche photodiode (APD) with a separate absorption, grading, charge, and multiplication (SAGCM) structure is epitaxially grown by molecular beam epitaxy (MBE). The resulting material is studied using X-ray diffraction (XRD), photoluminescence (PL), and scanning transmission electron microscopy. The activation energy extracted from the dark current of the APD indicates that it is dominated by the generation–recombination (G–R) process. Deep low-temperature PL peaks reveal the existence of an <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${E}_{v} + 0.42$ </tex-math></inline-formula> -eV deep energy level defect in the indium–gallium–arsenide (InGaAs) absorber layer, which is considered to be a result of point defects caused by Ga-poor or In-poor MBE growth conditions. The effect of the defect on the dark current is confirmed using numerical calculation methods.

Ground states and thermodynamics of the spin–electron model with mixed spins: Application to rare-earth tetraborides

A simple, but very realistic, spin–electron model is used to study the influence of mixed spins (from electron and spin subsystems) on a formation of fractional magnetization plateaus in rare-earth tetraborides. The spin subsystem is described by the ordinary Ising model and the electron subsystem by the ordinary Hubbard model. Moreover, both subsystems are coupled by the anisotropic spin-dependent interaction of the Ising type. To model the most realistically situation in rare-earth compounds we study the following combination of mixed spins: S = 1 , 3 / 2 and 2 in the spin subsystem and s d = 1 / 2 in the electron subsystem. It is shown that the mixed spins, in a combination with the Coulomb interaction U , have the significant impact on the formation and stabilization of different magnetization plateaus. In particular, we have found that the Coulomb interaction for S = 1 and S = 3 / 2 stabilizes the 1/2 plateau and strongly suppresses the 1/3 plateau which is in perfect agreement with the experimental measurements in TmB 4 and ErB 4 compounds. At nonzero temperatures our numerical results predict one high-temperature peak (of the Ising type) in the temperature dependence of the specific heat capacity, which accords with specific heat capacity measurements in TmB 4 and ErB 4 , and one low-temperature electron peak, which is not, however, seen in experiments. The reason is probably the fact that the electron peak appears at a several times lower temperature than the spin peak and thus the experiments, made only to 2 K, did not catch it. • A new spin–electron model with mixed spins is proposed. • Mixed spins in a combination with the Coulomb interaction stabilize 1/2 plateau. • Specific heat curves exhibit single- and double-peaked structure. • Predictions of our model are in a very good agreement with experiments in TmB 4 and ErB 4 .

Desorption characteristics of selenium and tellurium thin films

The temperature-dependent desorption behavior of selenium and tellurium is investigated using a heated quartz crystal microbalance. Prior to heating the quartz crystal microbalance, selenium and tellurium films with varying thickness were deposited using thermal effusion cells in a molecular beam epitaxy system for subsequent determination of temperature-dependent mass loss of the deposited films. The desorption rate for tellurium was found to exhibit one sharp peak around 190 °C, indicating the loss of the entire film irrespective of film thickness within a temperature window of 20 °C, which was completely evaporated at 200 °C. Similar experiments for selenium revealed that the thermal desorption took place via a two-stage process with a smaller portion of the material desorbing within an even narrower temperature window of 5 °C at a much lower peak temperature of 65 °C, while most selenium desorbed within a temperature range of 10 °C around 90 °C. This two-stage behavior indicated the presence of at least two chemically distinct selenium species or binding states. The direct and quantitative determination of the chalcogen desorption process provides important insights into the kinetics of chalcogenide-based film growth and is in addition of applied benefit to the research community in the area of Se/Te capping and decapping of air sensitive materials as it provides temperature ranges and rates at which full desorption is achieved. Our work furthermore points toward the need for a more detailed understanding of the chemical composition state of atomic and molecular beams supplied from thermal evaporation sources during growth.

Ground state and thermodynamic properties of the coupled double-Ising model: application to rare-earth tetraborides

A combination of the standard Metropolis algorithm and the parallel tempering method is used to study ground-state and thermodynamic properties of the coupled double Ising (CDI) model on the Shastry–Sutherland lattice (SSL). This model is derived from the complex spin-electron model, in which electrons described by the Hubbard model and spins described by the Ising model interact via the anisotropic spin-dependent interaction of the Ising type, under the following three conditions: (a) the Hubbard interaction between electrons in the conduction band is sufficiently large; (b) the number of conduction electrons is equal to the number of the lattice points; (c) there is the easy axis spin anisotropy in the system. The model is solved numerically for the selected combinations of spins from the electron () and spin () Ising branch which represent very realistically the situation in TmB4, ErB4 and HoB4 compounds, where in addition all three conditions are simultaneously satisfied. It is shown that the interlpay between the electron and spin branch of the CDI model leads to the suppression of the 1/3 magnetization plateau (the main magnetization plateau found in the ordinary Ising model on the SSL) and the stabilization of magnetization plateaus with , which is in perfect agreement with the experimental measurements in TmB4 and ErB4 compounds. A nice correspondence between theoretical and experimental results is also obtained for the temperature dependence of the specific heat capacity, where the low-temperature peak corresponding to the electron branch of the CDI model is followed by high-temperature peak of the spin branch. This opens a new route for exploring the physics of other complex spin-electron systems in which the above-mentioned conditions (a)–(c) are fulfilled.

Magnon drag induced by magnon-magnon interactions characteristic of noncollinear magnets

A noncollinear magnet consists of the magnetic moments forming a noncollinear spin structure. Because of this structure, the Hamiltonian of magnons acquires the cubic terms. Although the cubic terms are the magnon-magnon interactions characteristic of noncollinear magnets, their effects on magnon transport have not been clarified yet. Here we show that in a canted antiferromagnet the cubic terms cause a magnon drag that magnons drag magnon spin current and heat current, which can be used to enhance these currents by tuning a magnetic field. For a strong magnetic field, we find that the cubic terms induce low-temperature peaks of a spin-Seebeck coefficient, a magnon conductivity, and a magnon thermal conductivity, and that each value is one order of magnitude larger than the noninteracting value. This enhancement is mainly due to the magnetic field dependence of the coupling constant of the cubic terms through the magnetic-field dependent canting angle. Our magnon drag offers a way for controlling the magnon currents of noncollinear magnets via the many-body effect.

High oleic sunflower oil and fully hydrogenated soybean oil nanostructured lipid carriers: Development and characterization

Lipid-based nanoparticles are among the most promising encapsulation technologies in the field of nanotechnology. As one of the main trends in the development of these structures, the use of edible and/or commercially available oils and fats in the food industry stands out, replacing synthetic lipid matrices, which are not as viable for food applications in terms of cost, availability, or regulatory aspects. The objective of this work was to obtain and characterize nanostructured lipid carriers (NLC) using fully hydrogenated soybean oil (FHSO) and high oleic sunflower oil (HOSO) as lipid matrices. NLC were formulated from different lipid systems, 80:20, 60:40, 40:60, and 20:80 FHSO:HOSO (w/w), using soy lecithin (SL), Tween 80, or whey protein isolate (WPI) as an emulsifier. The increase in the unsaturation degree of the FHSO:HOSO lipid system resulted in larger NLC when obtained with Tween 80 or SL, greater physical instability, and lower peak temperature and melting enthalpy. The increase in the unsaturation degree, however, did not change the polymorphic shape of NLC, which stabilized in the β form 48 h after their obtainment. Among the considered lipid systems, 80:20, 60:40, and 40:60 FHSO:HOSO (w/w) systems form stable particles, with crystallinity properties suitable for food incorporation.

2D metal-organic frameworks endow ammonium perchlorate with enhanced thermal effect

To investigate the effect of different structures of MOF on the catalytic performance of ammonium perchlorate (AP) thermal decomposition. By adding 2-methylimidazole (2-MI) as an inhibitor during the synthesis of MOF-5, a two-dimensional (2D) MOF material was prepared and characterized by SEM, EDS, XRD, FT-IR and other means. The prepared two-dimensional material was added to the AP raw material to investigate its effect on the AP thermal decomposition process. After DSC and TG test, it was found that the addition of this kind of 2D MOF material can completely eliminate the low-temperature decomposition peak of the AP-based composite and advance the high temperature decomposition peak to 296.5 °C, and the apparent heat of decomposition increase to 905.6 J/g, which has a better catalytic effect than the bulk MOF-5. In addition, through the combustion test, it was found that 2D MOF, as a burning rate catalyst, can effectively enhance the burning rate of AP based solid propellant.

Dosimetric and TL investigation of natural and heat-treated Pakistani Onyx at high beta doses

Extensive Thermoluminescence (TL) glow curve analysis of natural (S1) and heat-treated (S4) Pakistani Onyx marble is reported exploring an alternative natural radiation dosimeter. TL curves for β-doses ranging from 0.5 Gy to 10 kGy are measured within the temperature range of 25–500 °C and analyzed to generate dose response curves (DRCs). Single saturation exponential function and DRCs are used to evaluate the characteristic dose value and the intensity saturation level. The glow peak repeatability test identifies unstable TL trapping sites in S1 at high temperatures (≥350 °C). Fading analysis of S4 shows that a major signal loss (40%) occurs within 24 h because of low temperature (<130 °C) peaks. After irradiation, time-temperature investigations are performed to optimize the pre-heat condition and remove fast fading peaks. The kinetic parameters are estimated using the TM-Tstop technique and the curve deconvolution method. The post-irradiation preheat at 100 °C for 10 s and TL data collection up to 400 °C with a heating rate of 5 °C/s is concluded as appropriate measurement condition to perform dosimetric studies of S4. The quantitative analysis of S4 dose response showed a linear behavior from 2 to 20 Gy, supra-linear from 20 to 5000 Gy, and sublinear response after 5–10 kGy. The minimum detectable dose (MDD) and percentage coefficient of variation (COV) of repeatability for S4 are 236 ± 8 mGy and 1.53% respectively. The study concludes that Pakistani Onyx marble, with thermal treatment of 500 °C for 1 h, can be a radiation dosimeter for high dose applications.

The effect of Fe-doping in magnetic properties of frustrated spinel CoAl2O4

In this work, we study the effect of Fe-doping in the magnetic properties of CoAl 2 O 4 , which presents a very high level of frustration. Samples are synthesized via solid state reaction by mixing stoichiometric amounts of CoO, Fe 2 O 3 and Al 2 O 3 starting oxides. The analysis of X-ray data show that our samples are single phase with cubic symmetry and space group f d − 3 m . A decrease of lattice parameter as a function of iron concentration is also inferred from the X-ray data. As compared with the pure sample, temperature dependence of magnetization of doped samples show an additional phase transition at high temperature. The enhancement of thermal hysteresis effect and the increasing of the Curie-Weiss temperatures with the Fe-doping can be an indicative of magnetic phase competition leading to a frustrated ground state. Indeed, the unsaturated state of the M v s H loops measured at T = 2 K is consistent with the strong frustration phenomenon. Finally, we argue that the displace of the low temperature peak, which is associated with the freezing temperature in the pure sample, into high temperature region as a function of Fe-doping can be relieving the frustration effect due the next-nearest-neighbor antiferromagnetic interaction J 2 . • Increase of lattice parameters a function of iron concentration. • Fe-doping the highly frustrated material CoAl 2 O 4 . • Magnetic phase competition in low temperature region.

Experimental Investigation on Effects of Fuel Injection Timings on Dimethyl Ether (DME) Energy Share Improvement and Emission Reduction in a Dual-Fuel CRDI Compression Ignition Engine

The impacts of different fuel injection timings (base (15BTDC) and retarded (12BTDC)) on a single cylinder common rail direct injection (CRDI) compression ignition (CI) engine under dual fuel mode (DME-diesel) was examined at the maximum torque with the engine speed of 2200 rpm. The diesel (liquid) fuel was directly injected into the engine’s cylinder at the end of the compression stroke and Dimethyl ether (gas) fuel was injected into the intake system of the engine during the suction stroke. The maximum DME energy share (DME ES) with base injection timing (15BTDC) under controlled auto-ignition (CAI) is limited to 52%. Delayed injection timing prevents knock occurrence to a certain extent due to the lower peak combustion pressure and temperature. The DME energy share (DME ES) without knocking is extended to 58% with delayed injection timing (12BTDC). Three stages of combustion (low-temperature region, high-temperature region and diffusion combustion region) were observed under DME-diesel mode. The low-temperature region (LTR) occurs at the temperature range from 700–900 K whereas high-temperature region (HTR) was at the temperature beyond 1000 K. The cyclic variations with the coefficient of variation (COV) of the important parameters (peak in-cylinder pressure, peak rate of pressure rise and indicated mean effective pressure) were analyzed. NOx emission decreased along with zero smoke emission. However, the other emissions such as CO, HC increased marginally with retarded timing. The notable point emerged from this study is that the retarded injection timing is a promising strategy for enhancement of DME energy share with reduced emissions.

Investigation of static and dynamic magnetic properties of Ni0.85Mg0.15Cr2O4 nanoparticles

Ni0.85Mg0.15Cr2O4 nanoparticles with average particle size of 46 nm were synthesized by hydrothermal route. Rietveld refinement reveals single phase cubic crystal structure with lattice constant 8.3560(6) Å. Temperature variation of magnetization measurements suggests multiple magnetic transitions in the compound. The low temperature peak observed around 10 K is attributed to a surface cluster glass like transition based on detailed relaxation, memory effect, field and temperature dependent magnetization measurements. In contrast to the canted spin structure of bulk NiCr2O4, the core spin structure of the nanoparticle system is showing tendency towards collinear ferrimagnetism. This leads to the suppression of ordering of transverse (antiferromagnetic) components of magnetic structure as typically observed in bulk NiCr2O4. Various memory and relaxation protocols were followed in order to study the dynamics of the nanoparticles. We have observed asymmetric response of magnetic relaxation with respect to change in temperature below the glassy transition temperature.

The peculiar spectral evolution of the new X-ray transient MAXI J0637–430

ABSTRACT We studied the transient Galactic black hole candidate MAXI J0637−430 with data from Insight-HXMT, Swift, and XMM–Newton. The broad-band X-ray observations from Insight-HXMT help us constrain the power-law component. MAXI J0637–430 is located at unusually high Galactic latitude; if it belongs to the Galactic thick disc, we suggest a most likely distance ≲7 kpc. Compared with other black hole transients, MAXI J0637–430 is also unusual for other reasons: a fast transition to the thermal dominant state at the start of the outburst; a low peak temperature and luminosity (we estimate them at ≈0.7 keV and ≲0.1 times Eddington, respectively); a short decline time-scale; a low soft-to-hard transition luminosity (≲0.01 times Eddington). We argue that such properties are consistent with a small binary separation, short binary period (P ∼ 2 h), and low-mass donor star (M2 ∼ 0.2 M⊙). Moreover, spectral modelling shows that a single disc blackbody component is not a good fit to the thermal emission. Soft spectral residuals, and deviations from the standard $L_{\rm disc} \propto T_{\rm in}^4$ relation, suggest the need for a second thermal component. We propose and discuss various scenarios for such component, in addition to those presented in previous studies of this source. For example, a gap in the accretion disc between a hotter inner ring near the innermost stable orbit, and a cooler outer disc. Another possibility is that the second thermal component is the thermal plasma emission from an ionized outflow.

Thermal properties of polymethyl methacrylate vary depending on brand and type.

Polymethyl methacrylate(PMMA) is commonly used in orthopedic surgery and has several applications, most often for fixation of arthroplasty components. While its overall safety and tolerance are well described, less is known regarding the thermal properties of PMMA as it sets from a liquid to solid state, as well as the potential for osseous thermal necrosis. This study addresses potential variations in the setting time and maximum temperature of PMMA formulations in common use and explores the potential clinical implications of this variability.Seven commercially available formulations of PMMA that varied by brand and/or viscosity were obtained and prepared according to manufacturer's instructions. Peak temperature and duration were measured in controlled settings for each type and compared to previously described thresholds for thermal bone necrosis.Depuy SmartSet (HV), Zimmer Palacos R(HV), and Zimmer Palacos (LV) exceeded the 56°C threshold reported to potentially induce immediate osseous thermal necrosis. Additionally, Biomet Cobalt (MV) and Stryker Simplex P (MV) had lower peak temperatures but exceeded thermal necrosis thresholds due to curing duration. The lowest peak temperature was observed for Smith & Nephew Versabond (MV), which was significantly lower than all types except Depuy SmartSet (MV). Setting time was not significantly different among groups.There are significant differences in the thermal properties of PMMA formulations in current use. Selection of specific PMMA formulations represents an additional route of procedural optimization depending on the needs of the treating surgeon.

Thermodynamic signature of SU(4) spin-orbital liquid and symmetry fractionalization from Lieb-Schultz-Mattis theorem

The state-of-the-art numerical simulation of the SU(4) Heisenberg model on a honeycomb lattice reveals a characteristic peak-and-shoulder specific heat behavior. The low-temperature peak is associated with a color gap, which suggests the existence of a gapped symmetric ground state in this model.

Effect of the Thermal History on Macrostructure and Microstructure Development in High-Strength Steel Welds

The present work addresses the microstructural and macrostructural development in multipass welded joints. It focuses on multiple thermal cycles induced by successive deposition of welding passes. The local welding-related thermal history was related in detail to the evolution of austenite grains during the manufacturing of two high-strength low alloy steel welds. The analytical Rosenthal thermal model was used to identify the thermal cycles experienced within typical weld metal regions. Selected heat cycles were applied to laboratory specimens, taken from the same weld metal, to investigate microstructural evolution during the welding process. Heat cycle experiments, involving full austenitization, showed the persistence of columnar zones resulting from a memory effect of the prior austenite grains during the reverse transformation. Intercritical heat cycles led to white etching, softer regions with high fractions of retained austenite. They also showed that the memory of austenite grains was actually stored in elongated retained austenite particles that remained after complete welding. This memory effect vanished under high peak temperatures (typically, 130 °C higher than Ac3); this was linked to a competition between growth and merging of elongated, intragranular retained austenite particles, and growth of equiaxed, intergranular austenite particles. Finally, a low peak temperature promoted refined, harder final microstructures.

Si doping in MOCVD grown (010) β-(AlxGa1−x)2O3 thin films

In this work, the structural and electrical properties of metalorganic chemical vapor deposited Si-doped β-(AlxGa1−x)2O3 thin films grown on (010) β-Ga2O3 substrates are investigated as a function of Al composition. The room temperature Hall mobility of 101 cm2/V s and low temperature peak mobility (T = 65 K) of 1157 cm2/V s at carrier concentrations of 6.56 × 1017 and 2.30 × 1017 cm−3 are measured from 6% Al composition samples, respectively. The quantitative secondary ion mass spectroscopy (SIMS) characterization reveals a strong dependence of Si and other unintentional impurities, such as C, H, and Cl concentrations in β-(AlxGa1−x)2O3 thin films, with different Al compositions. Higher Al compositions in β-(AlxGa1−x)2O3 result in lower net carrier concentrations due to the reduction of Si incorporation efficiency and the increase of C and H impurity levels that act as compensating acceptors in β-(AlxGa1−x)2O3 films. Lowering the growth chamber pressure reduces Si concentrations in β-(AlxGa1−x)2O3 films due to the increase of Al compositions as evidenced by comprehensive SIMS and Hall characterizations. Due to the increase of lattice mismatch between the epifilm and substrate, higher Al compositions lead to cracking in β-(AlxGa1−x)2O3 films grown on β-Ga2O3 substrates. The (100) cleavage plane is identified as a major cracking plane limiting the growth of high-quality Si-doped (010) β-(AlxGa1−x)2O3 films beyond the critical thicknesses, which leads to highly anisotropic and inhomogeneous behaviors in terms of conductivity.

Heat Source Modeling and Residual Stress Analysis for Metal Directed Energy Deposition Additive Manufacturing.

The advancement in additive manufacturing encourages the development of simplified tools for deep and swift research of the technology. Several approaches were developed to reduce the complexity of multi-track modeling for additive manufacturing. In the present work, a simple heat source model called concentrated heat source was evaluated for single- and multi-track deposition for directed energy deposition. The concentrated heat source model was compared with the widely accepted Goldak heat source model. The concentrated heat source does not require melt pool dimension measurement for thermal model simulation. Thus, it reduces the considerable time for preprocessing. The shape of the melt pool and temperature contour around the heat source was analyzed for single-track deposition. A good agreement was noticed for the concentrated heat source model melt pool, with an experimentally determined melt pool, using an optical microscope. Two heat source models were applied to multi-track 3D solid structure thermo-mechanical simulation. The results of the two models, for thermal history and residual stress, were compared with experimentally determined data. A good agreement was found for both models. The concentrated heat source model reported less than the half the computational time required for the Goldak model. The validated model, for 3D solid structure thermo-mechanical simulation, was used to analyze thermal stress evolution during the deposition process. The material deposition on the base plate at room temperature results in lower peak temperatures in the layers near the base plate. Consequently, the higher thermal stress in the layers near the base plate was found, compared to the upper layers during the deposition process.

Mechanics of solder/IMC interface of lead-free solder interconnects in ball grid array assembly

The lead-free Sn-0.4Ag-0.5Cu (SAC405) solder arrays provides an interconnection between the electronic package and printed circuit board (PCB) of the assembly. The ball grid array (BGA) test assembly was exposed to thermo-mechanical loading during solder reflow cooling and subsequent reliability temperature cycles. This could contribute to the solder/IMC interface damage and cracking. Finite element (FE) analysis was utilized to model the BGA assembly under the prescribed temperature loading profile. The unified constitutive (Anand) model was used to describe the temperature- and strain rate-dependent response, and solder/IMC interface damage of the SAC405 solder interconnects. Solder reflow cooling begins from the assumed stress-free reflow temperature of 220 °C to 25 °C at 1.3 °C/s. This was followed by temperature cycling between 125 and -40 °C with 15 minutes dwell time at upper and lower peak temperature levels. The temperature ramp rate of 11 °C/min was used. Results show that the most critically stressed solder joint was the one located underneath the edge of the silicon die. The solder/IMC interface crack initiated at the interface near the package side of the assembly. Catastrophic fracture of the BGA assembly was predicted during the first temperature cycle due to the relatively low input strength and toughness of the brittle-like solder/IMC interface properties. The solder/IMC failure prediction could not be inferred solely from inelastic strain in the bulk solder joint but should also consider the damage of the interface. This study shall benefit the newly designed BGA packages through rapid generation of reliability data and by providing insight into the reliability aspects of the BGA assembly with interface fracture issues.

Impact of extraction methods on functional properties and extraction kinetic of insoluble dietary fiber from green pea peels: A comparative analysis

The present study focused on the utilization of green pea peel (GPP) by-product for its insoluble dietary fiber (IDF) which was estimated by employing different extraction techniques. A comparative evaluation using various extraction methods viz., alkaline extraction, ultrasound-assisted extraction, and ultrasound-assisted alkaline extraction method (ODF) was employed vis-à-vis its effect on yield, kinetics, thermal stability, morphological, and functional properties of IDF. Ultrasound-assisted alkali extraction method was optimized to extract IDF and was found to be the best extraction method and standardized using rotatable central composite design with time of 30 min, amplitude of 30%, solid to liquid ratio (1:20), and NaOH concentration 1.2 mol/L. ODF evinced biologically rich and higher water and oil holding capacities with low peak and final transition temperature. The morphology of IDF also varied distinctly with extraction processes. ODF conclusively evidenced that it has immense potential to scale up in fulfilling the commercial demand of IDF. Novelty impact statement The pea peel insoluble dietary fiber (IDF) has enormous potential in food processing industries in developing functional foods which could unleash health benefit properties. The utilization could also minimize the environmental footprint of food wastage and disposal issues. The developed IDF from green pea peel (GPP) has enormous economic feasibility among various commercial food sectors viz., beverage, dairy, meat, and other health-promoting food industries. Extraction of IDF by a suitable extraction method from GPP by-product which was discarded largely hitherto has immense potential of generating substantial economic benefits every year and it can be an innovative approach for generating functional food ingredients.