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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59045 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | 1.4756 | 1.6887 | 0.8738 | [X:[], M:[0.9858, 0.9858], q:[0.4998, 0.4856], qb:[0.5144, 0.4718], phi:[0.3381]] | [X:[], M:[[-3, 3], [-3, 3]], q:[[-6, -3], [-9, 0]], qb:[[9, 0], [0, 9]], phi:[[1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}$ | -3 | t^2.03 + t^2.87 + t^2.91 + 2*t^2.96 + t^3. + t^3.89 + t^3.93 + t^4.01 + 2*t^4.06 + 2*t^4.9 + 2*t^4.94 + 2*t^4.99 + 2*t^5.03 + t^5.07 + t^5.39 + t^5.43 + t^5.47 + t^5.52 + t^5.74 + t^5.79 + 3*t^5.83 + 2*t^5.87 + 5*t^5.91 + 2*t^5.96 - 3*t^6. + 2*t^6.09 - t^6.13 + t^6.4 + t^6.44 + t^6.48 + t^6.53 + t^6.76 + 2*t^6.8 + 3*t^6.84 + 3*t^6.89 + 5*t^6.93 + 4*t^6.97 + 2*t^7.01 + 2*t^7.06 + t^7.1 - t^7.14 + t^7.29 + 2*t^7.42 + t^7.46 + t^7.5 + 2*t^7.54 + t^7.67 + 3*t^7.77 + 4*t^7.82 + 6*t^7.86 + 5*t^7.9 + 9*t^7.94 + 4*t^7.99 - 2*t^8.03 + t^8.07 + 3*t^8.11 - 2*t^8.16 + t^8.26 + 2*t^8.3 + 2*t^8.34 + t^8.35 + 2*t^8.38 + t^8.39 + 3*t^8.43 + t^8.47 - t^8.52 - t^8.56 - 2*t^8.6 + t^8.62 - t^8.64 + t^8.66 + 3*t^8.7 + 3*t^8.74 + 7*t^8.79 + 7*t^8.83 + 4*t^8.87 + t^8.91 + t^8.96 - t^4.01/y - t^5.03/y - t^6.04/y - t^6.89/y - t^6.93/y - (2*t^6.97)/y - t^7.01/y - t^7.06/y + t^7.99/y - t^8.07/y + t^8.79/y + (2*t^8.83)/y + (3*t^8.87)/y + t^8.91/y + t^8.96/y - t^4.01*y - t^5.03*y - t^6.04*y - t^6.89*y - t^6.93*y - 2*t^6.97*y - t^7.01*y - t^7.06*y + t^7.99*y - t^8.07*y + t^8.79*y + 2*t^8.83*y + 3*t^8.87*y + t^8.91*y + t^8.96*y | (g1^2*t^2.03)/g2^2 + (g2^9*t^2.87)/g1^9 + (g2^6*t^2.91)/g1^6 + (2*g2^3*t^2.96)/g1^3 + t^3. + (g2^8*t^3.89)/g1^8 + (g2^5*t^3.93)/g1^5 + (g1*t^4.01)/g2 + (2*g1^4*t^4.06)/g2^4 + (2*g2^7*t^4.9)/g1^7 + (2*g2^4*t^4.94)/g1^4 + (2*g2*t^4.99)/g1 + (2*g1^2*t^5.03)/g2^2 + (g1^5*t^5.07)/g2^5 + g1^10*g2^17*t^5.39 + t^5.43/(g1^23*g2^4) + t^5.47/(g1^20*g2^7) + g1^19*g2^8*t^5.52 + (g2^18*t^5.74)/g1^18 + (g2^15*t^5.79)/g1^15 + (3*g2^12*t^5.83)/g1^12 + (2*g2^9*t^5.87)/g1^9 + (5*g2^6*t^5.91)/g1^6 + (2*g2^3*t^5.96)/g1^3 - 3*t^6. + (2*g1^6*t^6.09)/g2^6 - (g1^9*t^6.13)/g2^9 + g1^11*g2^16*t^6.4 + t^6.44/(g1^22*g2^5) + t^6.48/(g1^19*g2^8) + g1^20*g2^7*t^6.53 + (g2^17*t^6.76)/g1^17 + (2*g2^14*t^6.8)/g1^14 + (3*g2^11*t^6.84)/g1^11 + (3*g2^8*t^6.89)/g1^8 + (5*g2^5*t^6.93)/g1^5 + (4*g2^2*t^6.97)/g1^2 + (2*g1*t^7.01)/g2 + (2*g1^4*t^7.06)/g2^4 + (g1^7*t^7.1)/g2^7 - (g1^10*t^7.14)/g2^10 + g1^3*g2^24*t^7.29 + 2*g1^12*g2^15*t^7.42 + (2*t^7.46)/(g1^21*g2^6) - g1^15*g2^12*t^7.46 + (2*t^7.5)/(g1^18*g2^9) - g1^18*g2^9*t^7.5 + 2*g1^21*g2^6*t^7.54 + (g1^30*t^7.67)/g2^3 + (3*g2^16*t^7.77)/g1^16 + (4*g2^13*t^7.82)/g1^13 + (6*g2^10*t^7.86)/g1^10 + (5*g2^7*t^7.9)/g1^7 + (9*g2^4*t^7.94)/g1^4 + (4*g2*t^7.99)/g1 - (2*g1^2*t^8.03)/g2^2 + (g1^5*t^8.07)/g2^5 + (3*g1^8*t^8.11)/g2^8 - (2*g1^11*t^8.16)/g2^11 + g1*g2^26*t^8.26 + (g2^5*t^8.3)/g1^32 + g1^4*g2^23*t^8.3 + (2*g2^2*t^8.34)/g1^29 + g1^7*g2^20*t^8.35 + (2*t^8.38)/(g1^26*g2) + g1^10*g2^17*t^8.39 + t^8.43/(g1^23*g2^4) + 2*g1^13*g2^14*t^8.43 + t^8.47/(g1^20*g2^7) - g1^19*g2^8*t^8.52 - (2*t^8.56)/(g1^14*g2^13) + g1^22*g2^5*t^8.56 - t^8.6/(g1^11*g2^16) - g1^25*g2^2*t^8.6 + (g2^27*t^8.62)/g1^27 - (g1^28*t^8.64)/g2 + (g2^24*t^8.66)/g1^24 + (3*g2^21*t^8.7)/g1^21 + (3*g2^18*t^8.74)/g1^18 + (7*g2^15*t^8.79)/g1^15 + (7*g2^12*t^8.83)/g1^12 + (4*g2^9*t^8.87)/g1^9 + (g2^6*t^8.91)/g1^6 + (g2^3*t^8.96)/g1^3 - (g1*t^4.01)/(g2*y) - (g1^2*t^5.03)/(g2^2*y) - (g1^3*t^6.04)/(g2^3*y) - (g2^8*t^6.89)/(g1^8*y) - (g2^5*t^6.93)/(g1^5*y) - (2*g2^2*t^6.97)/(g1^2*y) - (g1*t^7.01)/(g2*y) - (g1^4*t^7.06)/(g2^4*y) + (g2*t^7.99)/(g1*y) - (g1^5*t^8.07)/(g2^5*y) + (g2^15*t^8.79)/(g1^15*y) + (2*g2^12*t^8.83)/(g1^12*y) + (3*g2^9*t^8.87)/(g1^9*y) + (g2^6*t^8.91)/(g1^6*y) + (g2^3*t^8.96)/(g1^3*y) - (g1*t^4.01*y)/g2 - (g1^2*t^5.03*y)/g2^2 - (g1^3*t^6.04*y)/g2^3 - (g2^8*t^6.89*y)/g1^8 - (g2^5*t^6.93*y)/g1^5 - (2*g2^2*t^6.97*y)/g1^2 - (g1*t^7.01*y)/g2 - (g1^4*t^7.06*y)/g2^4 + (g2*t^7.99*y)/g1 - (g1^5*t^8.07*y)/g2^5 + (g2^15*t^8.79*y)/g1^15 + (2*g2^12*t^8.83*y)/g1^12 + (3*g2^9*t^8.87*y)/g1^9 + (g2^6*t^8.91*y)/g1^6 + (g2^3*t^8.96*y)/g1^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57648 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.4759 | 1.6899 | 0.8734 | [X:[], M:[0.9832, 0.9832], q:[0.5084, 0.4748], qb:[0.5084, 0.4748], phi:[0.3389]] | t^2.03 + t^2.85 + 4*t^2.95 + t^3.87 + 2*t^3.97 + 2*t^4.07 + 2*t^4.88 + 6*t^4.98 + t^5.08 + 2*t^5.39 + 2*t^5.49 + t^5.7 + 4*t^5.8 + 9*t^5.9 - 2*t^6. - t^4.02/y - t^5.03/y - t^4.02*y - t^5.03*y | detail |