DOI: 10.31274/etd-180810-1484
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Production and characterization of transgenic maize plants designed to improve iron nutrition

Abstract: The increasing need to find alternative solutions to the devastating effects of iron deficiency anemia has led to the generation of crops with improved nutritional quality traits. Iron is one of the required but limited mineral elements in most diets consumed by people in developing countries who have limited access to supplements or iron-rich diets. With much of the world's population dependent on maize as a major source of their daily calorie intake, research toward improving its nutritional value is deemed … Show more

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(3 citation statements)
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“…Extending the standard basis operator method developed by Haley and Erdös [15] to the boson Hubbard model, we calculate the superfluid density of states at T = 0. This method has been recently used by Sheshadri [7], Kanobe [16] and their coworkers to study the SI transition and the rf-spectrum in the Mott phase, respectively. In the superfluid phase near the SI transition, we show the coexistence of the itinerant gapless Bogoliubov mode and a band with a finite threshold energy, which reflects the localized character of atomic states.…”
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confidence: 99%
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“…Extending the standard basis operator method developed by Haley and Erdös [15] to the boson Hubbard model, we calculate the superfluid density of states at T = 0. This method has been recently used by Sheshadri [7], Kanobe [16] and their coworkers to study the SI transition and the rf-spectrum in the Mott phase, respectively. In the superfluid phase near the SI transition, we show the coexistence of the itinerant gapless Bogoliubov mode and a band with a finite threshold energy, which reflects the localized character of atomic states.…”
mentioning
confidence: 99%
“…∆E n−1,n may be regarded as the energy to add a hole to the ground state. The SI transition is determined by the condition when (8) has a gapless excitation at p = 0, which gives [3,7,9,16] The lowest value of U/zt to realize the Mott phase equals U/zt = 3 + 2 √ 2 = 5.83 (n = 1) [1,7,9]. We show the SI phase boundary given by (10) in Fig.…”
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