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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6719 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{5}M_{7}$ + ${ }M_{5}M_{8}$ + ${ }M_{6}M_{9}$ | 0.5953 | 0.7562 | 0.7872 | [M:[0.8541, 1.1424, 0.8611, 0.7135, 1.0018, 1.2865, 0.9982, 0.9982, 0.7135], q:[0.8594, 0.2865], qb:[0.4271, 0.7118], phi:[0.4288]] | [M:[[12], [2], [-16], [3], [-7], [-3], [7], [7], [3]], q:[[-9], [-3]], qb:[[6], [10]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{9}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }M_{8}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{9}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{9}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{9}$, ${ }M_{8}M_{9}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{1}M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{9}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{9}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{1}M_{2}$, ${ }M_{7}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{9}\phi_{1}\tilde{q}_{1}^{2}$ | ${}$ | -3 | 2*t^2.141 + t^2.562 + t^2.583 + 2*t^2.995 + 2*t^3.427 + t^3.849 + 3*t^4.281 + 2*t^4.703 + t^4.714 + 2*t^4.724 + t^5.125 + 4*t^5.135 + t^5.146 + t^5.167 + 2*t^5.557 + 3*t^5.568 + t^5.578 + 6*t^5.989 - 3*t^6. + t^6.011 + t^6.411 + 6*t^6.422 - t^6.432 + 4*t^6.844 + t^6.854 + t^6.865 + 2*t^7.265 + 7*t^7.276 - t^7.286 + 2*t^7.307 + t^7.687 + 5*t^7.698 + 5*t^7.708 + t^7.729 + t^7.75 + 2*t^8.12 + 9*t^8.13 - 5*t^8.141 + t^8.162 + 6*t^8.552 + 4*t^8.562 - t^8.573 - 3*t^8.583 + t^8.594 + t^8.974 + 10*t^8.984 - 6*t^8.995 - t^4.286/y - t^6.427/y - t^6.849/y - t^6.87/y + t^7.292/y + (3*t^7.703)/y + (3*t^7.724)/y + (4*t^8.135)/y + (2*t^8.146)/y + (2*t^8.557)/y + (3*t^8.568)/y + (2*t^8.578)/y + (4*t^8.989)/y - t^4.286*y - t^6.427*y - t^6.849*y - t^6.87*y + t^7.292*y + 3*t^7.703*y + 3*t^7.724*y + 4*t^8.135*y + 2*t^8.146*y + 2*t^8.557*y + 3*t^8.568*y + 2*t^8.578*y + 4*t^8.989*y | 2*g1^3*t^2.141 + g1^12*t^2.562 + t^2.583/g1^16 + 2*g1^7*t^2.995 + 2*g1^2*t^3.427 + g1^11*t^3.849 + 3*g1^6*t^4.281 + 2*g1^15*t^4.703 + g1*t^4.714 + (2*t^4.724)/g1^13 + g1^24*t^5.125 + 4*g1^10*t^5.135 + t^5.146/g1^4 + t^5.167/g1^32 + 2*g1^19*t^5.557 + 3*g1^5*t^5.568 + t^5.578/g1^9 + 6*g1^14*t^5.989 - 3*t^6. + t^6.011/g1^14 + g1^23*t^6.411 + 6*g1^9*t^6.422 - t^6.432/g1^5 + 4*g1^18*t^6.844 + g1^4*t^6.854 + t^6.865/g1^10 + 2*g1^27*t^7.265 + 7*g1^13*t^7.276 - t^7.286/g1 + (2*t^7.307)/g1^29 + g1^36*t^7.687 + 5*g1^22*t^7.698 + 5*g1^8*t^7.708 + t^7.729/g1^20 + t^7.75/g1^48 + 2*g1^31*t^8.12 + 9*g1^17*t^8.13 - 5*g1^3*t^8.141 + t^8.162/g1^25 + 6*g1^26*t^8.552 + 4*g1^12*t^8.562 - t^8.573/g1^2 - (3*t^8.583)/g1^16 + t^8.594/g1^30 + g1^35*t^8.974 + 10*g1^21*t^8.984 - 6*g1^7*t^8.995 - t^4.286/(g1*y) - (g1^2*t^6.427)/y - (g1^11*t^6.849)/y - t^6.87/(g1^17*y) + t^7.292/(g1^8*y) + (3*g1^15*t^7.703)/y + (3*t^7.724)/(g1^13*y) + (4*g1^10*t^8.135)/y + (2*t^8.146)/(g1^4*y) + (2*g1^19*t^8.557)/y + (3*g1^5*t^8.568)/y + (2*t^8.578)/(g1^9*y) + (4*g1^14*t^8.989)/y - (t^4.286*y)/g1 - g1^2*t^6.427*y - g1^11*t^6.849*y - (t^6.87*y)/g1^17 + (t^7.292*y)/g1^8 + 3*g1^15*t^7.703*y + (3*t^7.724*y)/g1^13 + 4*g1^10*t^8.135*y + (2*t^8.146*y)/g1^4 + 2*g1^19*t^8.557*y + 3*g1^5*t^8.568*y + (2*t^8.578*y)/g1^9 + 4*g1^14*t^8.989*y |
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 |
---|---|---|---|---|---|---|---|---|---|
5170 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{5}M_{7}$ + ${ }M_{5}M_{8}$ | 0.5751 | 0.7179 | 0.801 | [M:[0.8569, 1.1428, 0.8575, 0.7142, 1.0002, 1.2858, 0.9998, 0.9998], q:[0.8574, 0.2858], qb:[0.4284, 0.7141], phi:[0.4286]] | t^2.143 + t^2.571 + t^2.573 + 2*t^3. + 2*t^3.428 + t^3.856 + t^3.857 + t^4.285 + t^4.713 + t^4.714 + t^4.715 + t^5.141 + 2*t^5.142 + t^5.143 + t^5.145 + 2*t^5.57 + t^5.571 + t^5.572 + 5*t^5.999 - 2*t^6. - t^4.286/y - t^4.286*y | detail |