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 |
|---|---|---|---|---|---|---|---|---|---|
| 46025 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ | 0.5895 | 0.742 | 0.7945 | [M:[1.0406, 0.9189, 1.0], q:[0.5406, 0.5406], qb:[0.7601, 0.2399], phi:[0.4797]] | [M:[[0, -4], [0, 8], [0, 0]], q:[[-1, -8], [1, 0]], qb:[[0, -1], [0, 1]], phi:[[0, 2]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}^{3}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{2}\tilde{q}_{2}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | ${}$ | -4 | 2*t^2.341 + t^2.757 + t^2.878 + t^3. + t^3.122 + 2*t^3.78 + 2*t^3.902 + 6*t^4.683 + 2*t^5.22 + 2*t^5.341 + 2*t^5.463 + t^5.513 + t^5.635 + 2*t^5.757 + t^5.878 - 4*t^6. + 4*t^6.122 + 4*t^6.243 + 2*t^6.659 + 10*t^7.024 - 2*t^7.439 + 4*t^7.561 + 6*t^7.683 + 6*t^7.804 + 2*t^8.098 + t^8.27 - 10*t^8.341 + t^8.392 + 8*t^8.463 + 2*t^8.513 + 10*t^8.585 + 2*t^8.635 - t^8.757 - 5*t^8.878 - t^4.439/y - t^7.196/y + (2*t^7.683)/y + (2*t^8.098)/y + (2*t^8.22)/y + (2*t^8.341)/y + (2*t^8.463)/y + t^8.635/y + t^8.757/y + (2*t^8.878)/y - t^4.439*y - t^7.196*y + 2*t^7.683*y + 2*t^8.098*y + 2*t^8.22*y + 2*t^8.341*y + 2*t^8.463*y + t^8.635*y + t^8.757*y + 2*t^8.878*y | t^2.341/(g1*g2^7) + g1*g2*t^2.341 + g2^8*t^2.757 + g2^4*t^2.878 + t^3. + t^3.122/g2^4 + t^3.78/(g1*g2^5) + g1*g2^3*t^3.78 + t^3.902/(g1*g2^9) + (g1*t^3.902)/g2 + (2*t^4.683)/(g1^2*g2^14) + (2*t^4.683)/g2^6 + 2*g1^2*g2^2*t^4.683 + t^5.22/(g1*g2^3) + g1*g2^5*t^5.22 + t^5.341/(g1*g2^7) + g1*g2*t^5.341 + t^5.463/(g1*g2^11) + (g1*t^5.463)/g2^3 + g2^16*t^5.513 + g2^12*t^5.635 + 2*g2^8*t^5.757 + g2^4*t^5.878 - 2*t^6. - t^6./(g1^2*g2^8) - g1^2*g2^8*t^6. + t^6.122/(g1^2*g2^12) + (2*t^6.122)/g2^4 + g1^2*g2^4*t^6.122 + g1^2*t^6.243 + t^6.243/(g1^2*g2^16) + (2*t^6.243)/g2^8 + t^6.659/(g1*g2) + g1*g2^7*t^6.659 + (2*t^7.024)/(g1^3*g2^21) + (3*t^7.024)/(g1*g2^13) + (3*g1*t^7.024)/g2^5 + 2*g1^3*g2^3*t^7.024 - 2*g2^2*t^7.439 + (2*t^7.561)/(g1^2*g2^10) + 2*g1^2*g2^6*t^7.561 + (2*t^7.683)/(g1^2*g2^14) + (2*t^7.683)/g2^6 + 2*g1^2*g2^2*t^7.683 + (2*t^7.804)/(g1^2*g2^18) + (2*t^7.804)/g2^10 + (2*g1^2*t^7.804)/g2^2 + (g2*t^8.098)/g1 + g1*g2^9*t^8.098 + g2^24*t^8.27 - t^8.341/(g1^3*g2^15) - (4*t^8.341)/(g1*g2^7) - 4*g1*g2*t^8.341 - g1^3*g2^9*t^8.341 + g2^20*t^8.392 + (2*t^8.463)/(g1^3*g2^19) + (2*t^8.463)/(g1*g2^11) + (2*g1*t^8.463)/g2^3 + 2*g1^3*g2^5*t^8.463 + 2*g2^16*t^8.513 + (2*t^8.585)/(g1^3*g2^23) + (3*t^8.585)/(g1*g2^15) + (3*g1*t^8.585)/g2^7 + 2*g1^3*g2*t^8.585 + 2*g2^12*t^8.635 - g2^8*t^8.757 - t^8.878/(g1^2*g2^4) - 3*g2^4*t^8.878 - g1^2*g2^12*t^8.878 - (g2^2*t^4.439)/y - (g2^10*t^7.196)/y + (2*t^7.683)/(g2^6*y) + (g2*t^8.098)/(g1*y) + (g1*g2^9*t^8.098)/y + t^8.22/(g1*g2^3*y) + (g1*g2^5*t^8.22)/y + t^8.341/(g1*g2^7*y) + (g1*g2*t^8.341)/y + t^8.463/(g1*g2^11*y) + (g1*t^8.463)/(g2^3*y) + (g2^12*t^8.635)/y + (g2^8*t^8.757)/y + (2*g2^4*t^8.878)/y - g2^2*t^4.439*y - g2^10*t^7.196*y + (2*t^7.683*y)/g2^6 + (g2*t^8.098*y)/g1 + g1*g2^9*t^8.098*y + (t^8.22*y)/(g1*g2^3) + g1*g2^5*t^8.22*y + (t^8.341*y)/(g1*g2^7) + g1*g2*t^8.341*y + (t^8.463*y)/(g1*g2^11) + (g1*t^8.463*y)/g2^3 + g2^12*t^8.635*y + g2^8*t^8.757*y + 2*g2^4*t^8.878*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 |
|---|---|---|---|---|---|---|---|---|
| 46320 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 0.5742 | 0.7205 | 0.797 | [M:[1.1067, 0.7865, 1.0], q:[0.6699, 0.5436], qb:[0.7767, 0.2233], phi:[0.4466]] | t^2.301 + t^2.36 + 2*t^2.68 + t^3. + t^3.32 + t^3.64 + t^3.961 + t^4.02 + t^4.34 + 2*t^4.601 + t^4.719 + 3*t^4.98 + t^5.039 + t^5.301 + 5*t^5.36 + 2*t^5.68 + t^5.941 - t^6. - t^4.34/y - t^4.34*y | detail | |
| 46139 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ | 0.5867 | 0.74 | 0.7929 | [M:[1.0193, 0.9615, 1.0, 1.0193], q:[0.5193, 0.5193], qb:[0.7548, 0.2452], phi:[0.4904]] | 2*t^2.293 + t^2.884 + t^3. + 2*t^3.058 + 2*t^3.764 + 2*t^3.822 + 6*t^4.587 + 2*t^5.293 + 4*t^5.351 + t^5.769 + t^5.884 + t^5.942 - 5*t^6. - t^4.471/y - t^4.471*y | detail |
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 45882 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6849 | 0.8216 | 0.8337 | [M:[1.2094, 0.8921, 0.689], q:[0.554, 0.554], qb:[0.8024, 0.5086], phi:[0.3953]] | t^2.067 + t^2.676 + 2*t^3.188 + t^3.628 + 2*t^4.069 + t^4.134 + t^4.237 + 2*t^4.374 + 3*t^4.51 + t^4.743 + 2*t^5.255 + t^5.353 + t^5.695 - 5*t^6. - t^4.186/y - t^4.186*y | detail |