Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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56379 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{6}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | 0.641 | 0.8022 | 0.7991 | [M:[0.8947, 1.2105, 1.1053, 0.6843, 0.7895, 1.1053, 1.0001], q:[0.3421, 0.7632], qb:[0.4474, 0.5526], phi:[0.4737]] | [M:[[14], [10], [-14], [-34], [-10], [-14], [-38]], q:[[-17], [3]], qb:[[7], [31]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{1}$ | ${}M_{7}^{2}$ | -1 | t^2.053 + t^2.368 + t^2.842 + t^3. + 2*t^3.316 + t^3.474 + t^3.632 + t^3.79 + 2*t^4.105 + t^4.106 + 2*t^4.421 + 2*t^4.737 + t^4.895 + t^5.053 + t^5.211 + 2*t^5.369 + t^5.527 + 2*t^5.684 + 3*t^5.842 - t^6. + 5*t^6.158 + 4*t^6.474 - t^6.631 + 3*t^6.632 + 3*t^6.79 + 2*t^6.947 + 2*t^6.948 + 3*t^7.105 + t^7.106 + t^7.263 + 4*t^7.421 + 4*t^7.579 + 3*t^7.737 - t^7.894 + 4*t^7.895 + 2*t^8.21 + 6*t^8.211 - 5*t^8.368 + 3*t^8.369 + 4*t^8.526 + 2*t^8.527 + 4*t^8.842 - t^4.421/y - t^6.474/y + t^7.105/y - t^7.263/y + t^7.421/y + t^7.579/y - t^7.737/y + t^7.895/y + t^8.053/y + t^8.211/y + t^8.368/y + (3*t^8.369)/y + (3*t^8.684)/y + (3*t^8.842)/y - t^4.421*y - t^6.474*y + t^7.105*y - t^7.263*y + t^7.421*y + t^7.579*y - t^7.737*y + t^7.895*y + t^8.053*y + t^8.211*y + t^8.368*y + 3*t^8.369*y + 3*t^8.684*y + 3*t^8.842*y | t^2.053/g1^34 + t^2.368/g1^10 + t^2.842/g1^12 + t^3./g1^38 + (2*t^3.316)/g1^14 + t^3.474/g1^40 + g1^10*t^3.632 + t^3.79/g1^16 + 2*g1^8*t^4.105 + t^4.106/g1^68 + t^4.421/g1^44 + g1^32*t^4.421 + t^4.737/g1^20 + g1^56*t^4.737 + t^4.895/g1^46 + t^5.053/g1^72 + t^5.211/g1^22 + (2*t^5.369)/g1^48 + t^5.527/g1^74 + (2*t^5.684)/g1^24 + (3*t^5.842)/g1^50 - 2*t^6. + t^6./g1^76 + t^6.158/g1^102 + (4*t^6.158)/g1^26 + (3*t^6.316)/g1^52 - 3*g1^24*t^6.316 + (2*t^6.474)/g1^78 + (2*t^6.474)/g1^2 - g1^48*t^6.631 + (3*t^6.632)/g1^28 + (3*t^6.79)/g1^54 + (2*t^6.947)/g1^4 + (2*t^6.948)/g1^80 + (3*t^7.105)/g1^30 + t^7.106/g1^106 + (2*t^7.263)/g1^56 - g1^20*t^7.263 + (2*t^7.421)/g1^82 + (2*t^7.421)/g1^6 + t^7.579/g1^108 + (3*t^7.579)/g1^32 + (2*t^7.737)/g1^58 + g1^18*t^7.737 - g1^68*t^7.894 + (3*t^7.895)/g1^84 + t^7.895/g1^8 + t^8.053/g1^110 - t^8.053/g1^34 + 2*g1^16*t^8.21 + t^8.211/g1^136 + (5*t^8.211)/g1^60 - (5*t^8.368)/g1^10 + (3*t^8.369)/g1^86 + (3*t^8.526)/g1^36 + g1^40*t^8.526 + (2*t^8.527)/g1^112 + (4*t^8.684)/g1^62 - 4*g1^14*t^8.684 + (4*t^8.842)/g1^88 - (2*t^8.842)/g1^12 + 2*g1^64*t^8.842 - t^4.421/(g1^6*y) - t^6.474/(g1^40*y) + (g1^8*t^7.105)/y - t^7.263/(g1^18*y) + (g1^32*t^7.421)/y + (g1^6*t^7.579)/y - t^7.737/(g1^20*y) + t^7.895/(g1^46*y) + t^8.053/(g1^72*y) + t^8.211/(g1^22*y) + (g1^28*t^8.368)/y + (3*t^8.369)/(g1^48*y) + (3*t^8.684)/(g1^24*y) + (3*t^8.842)/(g1^50*y) - (t^4.421*y)/g1^6 - (t^6.474*y)/g1^40 + g1^8*t^7.105*y - (t^7.263*y)/g1^18 + g1^32*t^7.421*y + g1^6*t^7.579*y - (t^7.737*y)/g1^20 + (t^7.895*y)/g1^46 + (t^8.053*y)/g1^72 + (t^8.211*y)/g1^22 + g1^28*t^8.368*y + (3*t^8.369*y)/g1^48 + (3*t^8.684*y)/g1^24 + (3*t^8.842*y)/g1^50 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
52327 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{6}$ + ${ }\phi_{1}q_{2}^{2}$ | 0.6433 | 0.803 | 0.801 | [M:[0.8774, 1.1981, 1.1226, 0.7264, 0.8019, 1.1226], q:[0.3632, 0.7594], qb:[0.4387, 0.5142], phi:[0.4811]] | t^2.179 + t^2.406 + t^2.859 + t^2.887 + 2*t^3.368 + t^3.594 + t^3.622 + t^3.849 + 2*t^4.076 + t^4.302 + t^4.358 + t^4.529 + t^4.585 + t^4.811 + t^5.038 + t^5.066 + t^5.264 + t^5.292 + t^5.547 + t^5.717 + t^5.745 + 2*t^5.773 + t^5.802 - 2*t^6. - t^4.443/y - t^4.443*y | detail |