Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
46025 SU2adj1nf2 $M_1\phi_1^2$ + $ M_2q_1q_2$ + $ \phi_1\tilde{q}_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_3^2$ 0.5895 0.742 0.7945 [X:[], M:[1.0406, 0.9189, 1.0], q:[0.5406, 0.5406], qb:[0.7601, 0.2399], phi:[0.4797]] [X:[], M:[[0, -4], [0, 8], [0, 0]], q:[[-1, -8], [1, 0]], qb:[[0, -1], [0, 1]], phi:[[0, 2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ M_2$, $ \phi_1\tilde{q}_2^2$, $ M_3$, $ M_1$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ q_1\tilde{q}_1$, $ q_2\tilde{q}_1$, $ \phi_1q_1^2$, $ q_1^2\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ q_1q_2\tilde{q}_2^2$, $ \phi_1q_2^2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1q_1\tilde{q}_2^3$, $ \phi_1q_2\tilde{q}_2^3$, $ M_3q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_2$, $ M_1q_1\tilde{q}_2$, $ M_1q_2\tilde{q}_2$, $ M_2^2$, $ M_2\phi_1\tilde{q}_2^2$, $ M_2M_3$, $ \phi_1^2\tilde{q}_2^4$, $ M_1M_2$, $ M_3\phi_1\tilde{q}_2^2$ . -4 2*t^2.34 + t^2.76 + t^2.88 + t^3. + t^3.12 + 2*t^3.78 + 2*t^3.9 + 6*t^4.68 + 2*t^5.22 + 2*t^5.34 + 2*t^5.46 + t^5.51 + t^5.63 + 2*t^5.76 + t^5.88 - 4*t^6. + 4*t^6.12 + 4*t^6.24 + 2*t^6.66 + 10*t^7.02 - 2*t^7.44 + 4*t^7.56 + 6*t^7.68 + 6*t^7.8 + 2*t^8.1 + t^8.27 - 10*t^8.34 + t^8.39 + 8*t^8.46 + 2*t^8.51 + 10*t^8.58 + 2*t^8.63 - t^8.76 - 5*t^8.88 - t^4.44/y - t^7.2/y + (2*t^7.68)/y + (2*t^8.1)/y + (2*t^8.22)/y + (2*t^8.34)/y + (2*t^8.46)/y + t^8.63/y + t^8.76/y + (2*t^8.88)/y - t^4.44*y - t^7.2*y + 2*t^7.68*y + 2*t^8.1*y + 2*t^8.22*y + 2*t^8.34*y + 2*t^8.46*y + t^8.63*y + t^8.76*y + 2*t^8.88*y t^2.34/(g1*g2^7) + g1*g2*t^2.34 + g2^8*t^2.76 + g2^4*t^2.88 + t^3. + t^3.12/g2^4 + t^3.78/(g1*g2^5) + g1*g2^3*t^3.78 + t^3.9/(g1*g2^9) + (g1*t^3.9)/g2 + (2*t^4.68)/(g1^2*g2^14) + (2*t^4.68)/g2^6 + 2*g1^2*g2^2*t^4.68 + t^5.22/(g1*g2^3) + g1*g2^5*t^5.22 + t^5.34/(g1*g2^7) + g1*g2*t^5.34 + t^5.46/(g1*g2^11) + (g1*t^5.46)/g2^3 + g2^16*t^5.51 + g2^12*t^5.63 + 2*g2^8*t^5.76 + g2^4*t^5.88 - 2*t^6. - t^6./(g1^2*g2^8) - g1^2*g2^8*t^6. + t^6.12/(g1^2*g2^12) + (2*t^6.12)/g2^4 + g1^2*g2^4*t^6.12 + g1^2*t^6.24 + t^6.24/(g1^2*g2^16) + (2*t^6.24)/g2^8 + t^6.66/(g1*g2) + g1*g2^7*t^6.66 + (2*t^7.02)/(g1^3*g2^21) + (3*t^7.02)/(g1*g2^13) + (3*g1*t^7.02)/g2^5 + 2*g1^3*g2^3*t^7.02 - 2*g2^2*t^7.44 + (2*t^7.56)/(g1^2*g2^10) + 2*g1^2*g2^6*t^7.56 + (2*t^7.68)/(g1^2*g2^14) + (2*t^7.68)/g2^6 + 2*g1^2*g2^2*t^7.68 + (2*t^7.8)/(g1^2*g2^18) + (2*t^7.8)/g2^10 + (2*g1^2*t^7.8)/g2^2 + (g2*t^8.1)/g1 + g1*g2^9*t^8.1 + g2^24*t^8.27 - t^8.34/(g1^3*g2^15) - (4*t^8.34)/(g1*g2^7) - 4*g1*g2*t^8.34 - g1^3*g2^9*t^8.34 + g2^20*t^8.39 + (2*t^8.46)/(g1^3*g2^19) + (2*t^8.46)/(g1*g2^11) + (2*g1*t^8.46)/g2^3 + 2*g1^3*g2^5*t^8.46 + 2*g2^16*t^8.51 + (2*t^8.58)/(g1^3*g2^23) + (3*t^8.58)/(g1*g2^15) + (3*g1*t^8.58)/g2^7 + 2*g1^3*g2*t^8.58 + 2*g2^12*t^8.63 - g2^8*t^8.76 - t^8.88/(g1^2*g2^4) - 3*g2^4*t^8.88 - g1^2*g2^12*t^8.88 - (g2^2*t^4.44)/y - (g2^10*t^7.2)/y + (2*t^7.68)/(g2^6*y) + (g2*t^8.1)/(g1*y) + (g1*g2^9*t^8.1)/y + t^8.22/(g1*g2^3*y) + (g1*g2^5*t^8.22)/y + t^8.34/(g1*g2^7*y) + (g1*g2*t^8.34)/y + t^8.46/(g1*g2^11*y) + (g1*t^8.46)/(g2^3*y) + (g2^12*t^8.63)/y + (g2^8*t^8.76)/y + (2*g2^4*t^8.88)/y - g2^2*t^4.44*y - g2^10*t^7.2*y + (2*t^7.68*y)/g2^6 + (g2*t^8.1*y)/g1 + g1*g2^9*t^8.1*y + (t^8.22*y)/(g1*g2^3) + g1*g2^5*t^8.22*y + (t^8.34*y)/(g1*g2^7) + g1*g2*t^8.34*y + (t^8.46*y)/(g1*g2^11) + (g1*t^8.46*y)/g2^3 + g2^12*t^8.63*y + g2^8*t^8.76*y + 2*g2^4*t^8.88*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
46320 $M_1\phi_1^2$ + $ M_2q_1q_2$ + $ \phi_1\tilde{q}_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_3^2$ + $ M_1q_1\tilde{q}_2$ 0.5742 0.7205 0.797 [X:[], M:[1.1067, 0.7865, 1.0], q:[0.6699, 0.5436], qb:[0.7767, 0.2233], phi:[0.4466]] t^2.3 + t^2.36 + 2*t^2.68 + t^3. + t^3.32 + t^3.64 + t^3.96 + t^4.02 + t^4.34 + 2*t^4.6 + t^4.72 + 3*t^4.98 + t^5.04 + t^5.3 + 5*t^5.36 + 2*t^5.68 + t^5.94 - t^6. - t^4.34/y - t^4.34*y detail
46139 $M_1\phi_1^2$ + $ M_2q_1q_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 [X:[], M:[1.0193, 0.9615, 1.0, 1.0193], q:[0.5193, 0.5193], qb:[0.7548, 0.2452], phi:[0.4904]] 2*t^2.29 + t^2.88 + t^3. + 2*t^3.06 + 2*t^3.76 + 2*t^3.82 + 6*t^4.59 + 2*t^5.29 + 4*t^5.35 + t^5.77 + t^5.88 + t^5.94 - 5*t^6. - t^4.47/y - t^4.47*y detail


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
45882 SU2adj1nf2 $M_1\phi_1^2$ + $ M_2q_1q_2$ + $ \phi_1\tilde{q}_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ 0.6849 0.8216 0.8337 [X:[], M:[1.2094, 0.8921, 0.689], q:[0.554, 0.554], qb:[0.8024, 0.5086], phi:[0.3953]] t^2.07 + t^2.68 + 2*t^3.19 + t^3.63 + 2*t^4.07 + t^4.13 + t^4.24 + 2*t^4.37 + 3*t^4.51 + t^4.74 + 2*t^5.25 + t^5.35 + t^5.7 - 5*t^6. - t^4.19/y - t^4.19*y detail